Microstructure enhanced absorption photosensitive devices

ABSTRACT

Lateral and vertical microstructure enhanced photodetectors and avalanche photodetectors are monolithically integrated with CMOS/BiCMOS ASICs and can also be integrated with laser devices using fluidic assembly techniques. Photodetectors can be configured in a vertical PIN arrangement or lateral metal-semiconductor-metal arrangement where electrodes are in an inter-digitated pattern. Microstructures, such as holes and protrusions, can improve quantum efficiency in silicon, germanium and III-V materials and can also reduce avalanche voltages for avalanche photodiodes. Applications include optical communications within and between datacenters, telecommunications, LIDAR, and free space data communication.

REFERENCE TO RELATED APPLICATIONS

This application is a continuation-in-part of each of: U.S. patentapplication Ser. No. 16/042,535 filed Jul. 23, 2018; InternationalPatent Appl. No. PCT/US18/43289 filed Jul. 23, 2018 and published as WO2019/018846; U.S. patent application Ser. No. 15/797,821 filed Oct. 30,2017; U.S. patent application Ser. No. 14/947,718 filed Nov. 20, 2015;and International Patent Appl. No. PCT/US16/67977 filed Dec. 21, 2016published as WO 2017/112747; U.S. patent application. Ser. No.16/296,985 filed Mar. 8, 2019; and International Patent Appl. No.PCT/US18/57963 filed Oct. 29, 2018 and published as WO 2019/089437.

This application incorporates by reference and claims the benefit of thefiling date of each of the above-identified patent applications, as wellas of the applications that they incorporate by reference, directly orindirectly, and the benefit of which they claim, including U.S.provisional applications, U.S. non-provisional applications, andInternational applications.

This patent application claims the benefit of and incorporates byreference each of the following provisional applications:

U.S. Prov. Ser. No. 62/713,455 filed Aug. 1, 2018;

U.S. Prov. Ser. No. 62/716,310 filed Aug. 8, 2018;

U.S. Prov. Ser. No. 62/717,750 filed Aug. 10, 2018;

U.S. Prov. Ser. No. 62/719,689 filed Aug. 19, 2018;

U.S. Prov. Ser. No. 62/724,449 filed Aug. 29, 2018;

U.S. Prov. Ser. No. 62/733,476 filed Sep. 19, 2018;

U.S. Prov. Ser. No. 62/737,062 filed Sep. 26, 2018;

U.S. Prov. Ser. No. 62/750,016 filed Oct. 24, 2018;

U.S. Prov. Ser. No. 62/770,656 filed Nov. 21, 2018;

U.S. Prov. Ser. No. 62/772,498 filed Nov. 28, 2018;

U.S. Prov. Ser. No. 62/777,157 filed Dec. 9, 2018;

U.S. Prov. Ser. No. 62/779,693 filed Dec. 14, 2018;

U.S. Prov. Ser. No. 62/784,342 filed Dec. 21, 2018;

U.S. Prov. Ser. No. 62/794,330 filed Jan. 18, 2019;

U.S. Prov. Ser. No. 62/797,141 filed Jan. 25, 2019;

U.S. Prov. Ser. No. 62/797,263 filed Jan. 26, 2019;

U.S. Prov. Ser. No. 62/800,371 filed Feb. 1, 2019;

U.S. Prov. Ser. No. 62/802,171 filed Feb. 6, 2019;

U.S. Prov. Ser. No. 62/802,718 filed Feb. 8, 2019;

U.S. Prov. Ser. No. 62/805,850 filed Feb. 14, 2019;

U.S. Prov. Ser. No. 62/808,949 filed Feb. 22, 2019;

U.S. Prov. Ser. No. 62/819,604 filed Mar. 17, 2019;

U.S. Prov. Ser. No. 62/819,669 filed Mar. 17, 2019;

U.S. Prov. Ser. No. 62/820,695 filed Mar. 19, 2019;

U.S. Prov. Ser. No. 62/828,976 filed Apr. 3, 2019;

U.S. Prov. Ser. No. 62/841,798 filed May 1, 2019;

U.S. Prov. Ser. No. 62/843,206 filed May 3, 2019;

U.S. Prov. Ser. No. 62/846,554 filed May 10, 2019;

U.S. Prov. Ser. No. 62/853,280 filed May 29, 2019;

U.S. Prov. Ser. No. 62/860,115 filed Jun. 11, 2019;

U.S. Prov. Ser. No. 62/863,231 filed Jun. 18, 2019;

U.S. Prov. Ser. No. 62/863,852 filed Jun. 19, 2019;

U.S. Prov. Ser. No. 62/867,186 filed Jun. 26, 2019;

U.S. Prov. Ser. No. 62/868,911 filed Jun. 29, 2019;

U.S. Prov. Ser. No. 62/870,533 filed Jul. 3, 2019;

U.S. Prov. Ser. No. 62/873,891 filed Jul. 13, 2019, and

U.S. Prov. Ser. No. 62/874,418 filed Jul. 15, 2019.

Said U.S. patent application Ser. No. 16/296,985 is a continuation ofsaid U.S. patent application Ser. No. 15/797,821, and said U.S. patentapplication Ser. No. 16/042,535 is a continuation-in-part of said U.S.patent application Ser. No. 15/797,821.

Said U.S. patent application Ser. No. 15/797,821 claims the benefit ofand incorporates by reference each of the following provisionalapplications:

U.S. Prov. Ser. No. 62/465,734 filed Mar. 1, 2017;

U.S. Prov. Ser. No. 62/474,179 filed Mar. 21, 2017;

U.S. Prov. Ser. No. 62/484,474 filed Apr. 12, 2017;

U.S. Prov. Ser. No. 62/487,606 filed Apr. 20, 2017;

U.S. Prov. Ser. No. 62/488,998 filed Apr. 24, 2017;

U.S. Prov. Ser. No. 62/500,581 filed May 3, 2017;

U.S. Prov. Ser. No. 62/505,974 filed May 14, 2017;

U.S. Prov. Ser. No. 62/509,093 filed May 20, 2017;

U.S. Prov. Ser. No. 62/510,249 filed May 23, 2017;

U.S. Prov. Ser. No. 62/514,889 filed Jun. 4, 2017;

U.S. Prov. Ser. No. 62/521,504 filed Jun. 18, 2017;

U.S. Prov. Ser. No. 62/522,169 filed Jun. 20, 2017;

U.S. Prov. Ser. No. 62/527,962 filed Jun. 30, 2017;

U.S. Prov. Ser. No. 62/530,281 filed Jul. 9, 2017;

U.S. Prov. Ser. No. 62/533,078 filed Jul. 16, 2017;

U.S. Prov. Ser. No. 62/533,603 filed Jul. 17, 2017;

U.S. Prov. Ser. No. 62/535,801 filed Jul. 21, 2017;

U.S. Prov. Ser. No. 62/540,524 filed Aug. 2, 2017;

U.S. Prov. Ser. No. 62/542,243 filed Aug. 7, 2017;

U.S. Prov. Ser. No. 62/547,728 filed Aug. 18, 2017;

U.S. Prov. Ser. No. 62/553,844 filed Sep. 2, 2017;

U.S. Prov. Ser. No. 62/556,426 filed Sep. 10, 2017; and

U.S. Prov. Ser. No. 62/561,869 filed Sep. 22, 2017.

Said U.S. patent application Ser. No. 15/797,821 is acontinuation-in-part of each of:

-   -   U.S. patent application Ser. No. 15/309,922, filed Nov. 9, 2016,        now U.S. Pat. No. 9,818,893, which is a § 371 national stage of        International Patent Appl. No. PCT/US15/061120 filed Nov. 17,        2015;    -   Said U.S. patent application Ser. No. 14/947,718 filed Nov. 20,        2015; and    -   Said International Patent Appl. No. PCT/US16/67977 filed Dec.        21, 2016 published as WO2017/112747.

Said application Ser. No. 15/309,922 is a continuation of each of (i)U.S. patent application Ser. No. 14/943,898 (now U.S. Pat. No.9,530,905), (ii) U.S. patent application Ser. No. 14/945,003 filed Nov.18, 2011 (now U.S. Pat. No. 9,525,084), and is a § 371 national stage ofInternational Patent Appl. No. PCT/US15/061120, and incorporates each byreference and claims the benefit of the filing date of each as well asof each of the U.S. Provisional Patent applications the benefit of whichthey claim, including:

-   -   U.S. Prov. Ser. No. 62/081,538 filed Nov. 18, 2014;    -   U.S. Prov. Ser. No. 62/090,879 filed Dec. 11, 2014;    -   U.S. Prov. Ser. No. 62/100,025 filed Jan. 5, 2015;    -   U.S. Prov. Ser. No. 62/111,582 filed Feb. 3, 2015;    -   U.S. Prov. Ser. No. 62/139,511 filed Mar. 27, 2015;    -   U.S. Prov. Ser. No. 62/153,443 filed Apr. 27, 2015    -   U.S. Prov. Ser. No. 62/154,675 filed Apr. 29, 2015;    -   U.S. Prov. Ser. No. 62/157,876 filed May 6, 2015;    -   U.S. Prov. Ser. No. 62/171,915 filed Jun. 5, 2015;    -   U.S. Prov. Ser. No. 62/174,498 filed Jun. 11, 2015    -   U.S. Prov. Ser. No. 62/175,855 filed Jun. 15, 2015;    -   U.S. Prov. Ser. No. 62/182,602 filed Jun. 21, 2015;    -   U.S. Prov. Ser. No. 62/188,876 filed Jul. 6, 2015;    -   U.S. Prov. Ser. No. 62/197,120 filed Jul. 27, 2015;    -   U.S. Prov. Ser. No. 62/199,607 filed Jul. 31, 2015;    -   U.S. Prov. Ser. No. 62/205,717 filed Aug. 15, 2015;    -   U.S. Prov. Ser. No. 62/209,311 filed Aug. 24, 2015;    -   U.S. Prov. Ser. No. 62/213,556 filed Sep. 2, 2015; and    -   U.S. Prov. Ser. No. 62/232,716 filed Sep. 25, 2015.

Said application Ser. No. 14/947,718 is a continuation of InternationalPatent Appl. No. PCT/US14/39208, published as WO 2014/190189, andincorporates each by reference and claims the benefit of the filing datethereof and of each of the U.S. Provisional Patent applications thebenefit of which it claims including:

-   -   U.S. Prov. Ser. No. 61/826,446 filed May 22, 2013;    -   U.S. Prov. Ser. No. 61/834,873 filed Jun. 13, 2013;    -   U.S. Prov. Ser. No. 61/843,021 filed Jul. 4, 2013; and    -   U.S. Prov. Ser. No. 61/905,109 filed Nov. 15, 2013.

Said International Patent Appl. No. PCT/US16/67977 claims the benefit ofthe filing date of each of the following U.S. Provisional Patentapplications:

-   -   U.S. Prov. Ser. No. 62/270,577 filed Dec. 21, 2015;    -   U.S. Prov. Ser. No. 62/290,391 filed Feb. 2, 2016;    -   U.S. Prov. Ser. No. 62/304,907 filed Mar. 7, 2016;    -   U.S. Prov. Ser. No. 62/334,934 filed May 11, 2016;    -   U.S. Prov. Ser. No. 62/338,263 filed May 18, 2016;    -   U.S. Prov. Ser. No. 62/346,850 filed Jun. 7, 2016;    -   U.S. Prov. Ser. No. 62/359,349 filed Jul. 7, 2016;    -   U.S. Prov. Ser. No. 62/366,188 filed Jul. 25, 2016;    -   U.S. Prov. Ser. No. 62/368,109 filed Jul. 28, 2016;    -   U.S. Prov. Ser. No. 62/374,828 filed Aug. 13, 2016;    -   U.S. Prov. Ser. No. 62/376,869 filed Aug. 18, 2016;    -   U.S. Prov. Ser. No. 62/380,364 filed Aug. 27, 2016;    -   U.S. Prov. Ser. No. 62/383,391 filed Sep. 3, 2016;    -   U.S. Prov. Ser. No. 62/383,479 filed Sep. 4, 2016;    -   U.S. Prov. Ser. No. 62/394,222 filed Sep. 14, 2016;    -   U.S. Prov. Ser. No. 62/398,607 filed Sep. 23, 2016;    -   U.S. Prov. Ser. No. 62/401,126 filed Sep. 28, 2016;    -   U.S. Prov. Ser. No. 62/406,999 filed Oct. 12, 2016;    -   U.S. Prov. Ser. No. 62/414,671 filed Oct. 29, 2016; and    -   U.S. Prov. Ser. No. 62/415,339 filed Oct. 31, 2016.

Each of said PCT/US18/43289 filed Jul. 23, 2018 and said PCT/US18/57963filed Oct. 29, 2018 is a continuation-in-part of said U.S. patentapplication Ser. No. 15/797,821, and PCT/US18/43289 claims the benefitof and incorporates by reference each of the following provisionalapplications:

U.S. Prov. Ser. No. 62/535,801 filed Jul. 21, 2017;

U.S. Prov. Ser. No. 62/540,524 filed Aug. 2, 2017;

U.S. Prov. Ser. No. 62/542,243 filed Aug. 7, 2017;

U.S. Prov. Ser. No. 62/547,728 filed Aug. 18, 2017;

U.S. Prov. Ser. No. 62/553,844 filed Sep. 2, 2017;

U.S. Prov. Ser. No. 62/556,426 filed Sep. 10, 2017;

U.S. Prov. Ser. No. 62/561,869 filed Sep. 22, 2017;

U.S. Prov. Ser. No. 62/591,072 filed Nov. 27, 2017

U.S. Prov. Ser. No. 62/599,246 filed Dec. 15, 2017

U.S. Prov. Ser. No. 62/607,860 filed Dec. 19, 2017

U.S. Prov. Ser. No. 62/615,314 filed Jan. 9, 2018

U.S. Prov. Ser. No. 62/623,971 filed Jan. 30, 2018

U.S. Prov. Ser. No. 62/628,764 filed Feb. 9, 2018

U.S. Prov. Ser. No. 62/631,630 filed Feb. 17, 2018

U.S. Prov. Ser. No. 62/633,514 filed Feb. 21, 2018

U.S. Prov. Ser. No. 62/634,692 filed Feb. 23, 2018

U.S. Prov. Ser. No. 62/637,945 filed Mar. 2, 2018

U.S. Prov. Ser. No. 62/639,356 filed Mar. 6, 2018

U.S. Prov. Ser. No. 62/639,472 filed Mar. 6, 2018

U.S. Prov. Ser. No. 62/639,920 filed Mar. 7, 2018

U.S. Prov. Ser. No. 62/640,522 filed Mar. 8, 2018

U.S. Prov. Ser. No. 62/643,010 filed Mar. 14, 2018

U.S. Prov. Ser. No. 62/645,810 filed Mar. 21, 2018

U.S. Prov. Ser. No. 62/646,871 filed Mar. 22, 2018

U.S. Prov. Ser. No. 62/651,053 filed Mar. 30, 2018;

U.S. Prov. Ser. No. 62/651,087 filed Mar. 31, 2018;

U.S. Prov. Ser. No. 62/652,830 filed Apr. 4, 2018;

U.S. Prov. Ser. No. 62/659,067 filed Apr. 17, 2018;

U.S. Prov. Ser. No. 62/659,072 filed Apr. 17, 2018;

U.S. Prov. Ser. No. 62/662,217 filed Apr. 24, 2018;

U.S. Prov. Ser. No. 62/666,005 filed May 2, 2018;

U.S. Prov. Ser. No. 62/669,194 filed May 9, 2018;

U.S. Prov. Ser. No. 62/675,130 filed May 22, 2018;

U.S. Prov. Ser. No. 62/677,609 filed May 29, 2018; and

U.S. Prov. Ser. No. 62/682,909 filed Jun. 9, 2018.

All of the above-referenced provisional and non-provisional patentapplications are collectively referenced herein as “the commonlyassigned incorporated applications.”

FIELD

This patent specification relates mainly to photosensitive devices. Moreparticularly, some embodiments relate to photosensitive devices havingmicrostructure enhanced absorption characteristics and photosensitivedevices monolithically integrated with active electronic circuits on orin the same chip.

BACKGROUND

Fiber-optic communication is widely used in applications such astelecommunications, communication within large data centers, andcommunications between data centers. Because of attenuation lossesassociated with using shorter optical wavelengths, most fiber-optic datacommunication uses optical wavelengths of 800 nm and longer. Commonlyused multimode and single mode optical fiber uses wavelengths between800 nm and 1675 nm. A main component of optical receivers used infiber-optic communication system is the photo detector, usually in theform of a photodiode (PD) or avalanche photodiode (APO).

High-quality low-noise APDs can be made from silicon. However, whilesilicon will absorb light in the visible and near infrared range, itbecomes more transparent at longer optical wavelengths. Silicon PDs andAPDs can be made for optical wavelengths of 800 nm and longer byincreasing the thickness of the absorption “I” region of the device.However, in order to obtain adequate quantum efficiency (also known asexternal quantum efficiency), the thickness of the silicon “I” regionbecomes so large that the device's maximum bandwidth (also referred toas “data rate”) becomes too low for many current and future telecom anddata center applications.

To avoid the inherent problem that silicon PDs and APDs have with longerwavelengths and higher bandwidths, other materials are used. Germanium(Ge) APDs detect infrared out to a wavelength of 2000 nm, but haverelatively high multiplication noise. InGaAs APDs can detect out tolonger than 1600 nm, and have less multiplication noise than Ge, butstill far greater multiplication noise than silicon APDs. InGaAs isknown to be used as the absorption region of a heterostructure diode,most typically involving InP as a substrate and as a multiplicationlayer. This material system is compatible with an absorption window ofroughly 900 to 1700 nm. However, InGaAs PD and APO devices arerelatively expensive and have relatively high multiplication noise whencompared with silicon and are difficult to integrate with Si electronicsas a single chip.

Information published by a major company in the business ofphotodetectors (Seehttp://files.shareholder.com/downloads/FNSR/Ox0x382377/0b3893ea-fb06-417d-ac71-84f2f9084b0d/Finisar_Investor_Presentation.pdf,)indicates at page 10 that the current market for optical communicationdevices is over 7 billion U.S. dollars with a compounded annual growthrate of 12%. Photodiodes (PD) used for 850-950 nm wavelength employ GaAsmaterial and for 1550-1650 nm wavelength photodiodes are InP materialbased, which is both expensive and difficult to integrate with Si basedelectronics. Therefore, there is a large market and a long-felt needthat has not been met for the development of a better device. To datethere are no Si material based photodiodes nor avalanche photodiodes(APO) for 850-950 nm and no Ge on Si material based photodiodes noravalanche photodiodes for 1550-1650 nm that are top-surface orbottom-surface illuminated, with a data rate of at least 25 Gb/s, andare monolithically integrated with CMOS/BiCMOS silicon electronics on asingle chip that are commercially available, to the knowledge of theinventors herein. However, there has been no lack of trying to develop abetter device for this large market. For example, there have beenproposals for resonant photodiodes fabricated in Si material (seeResonant-Cavity-Enhanced High-Speed Si Photodiode Grown by EpitaxialLateral Overgrowth, Schaub et al., IEEE PHOTONICS TECHNOLOGY LETTERS,VOL. 11, NO. 12, December 1999), but they have not reached the knowncommercial market. Other forms of high speed photodiodes in a waveguideconfiguration have been proposed, such as in 40 GHz Si/Ge uni-travelingcarrier waveguide photodiode, Piels et al, DOI 10.1109/JLT.2014.2310780,Journal of Lightwave Technology (incorporated herein by reference);Monolithic germanium/silicon avalanche photodiodes with 340 GHzgain-bandwidth product, NATURE PHOTONICS | VOL 3 | January 2009 |www.nature.com/naturephotonics (incorporated herein by reference andreferred to herein as “Kong et al. 2009”); High-speed Ge photodetectormonolithically integrated with large cross-section silicon-on-insulatorwaveguide, Feng et al., Applied Physics Letters 95, 261105 (2009), doi:10.1063/1.3279129 (incorporated herein by reference); where light iscoupled edge-wise into an optical waveguide and where the absorptionlength can be 100 um or longer to compensate for the weak absorptioncoefficient of Ge at 1550 nm. In these previously proposed waveguidephotodiode structures, light propagates along the length of thewaveguide and the electric field is applied across the PIN waveguidesuch that the direction of light propagation and the direction of theelectric field are predominantly perpendicular in this waveguideconfiguration. Since light in Si travels approximately 1000 times fasterthan the saturated velocity of electrons/holes, a waveguide PD can be200 microns long for example and the “I” in the PIN can be 2 microns,for example, and achieve a bandwidth of over 10 Gb/s. Such edge couplingof light is costly in packaging as compared to surface illumination asdescribed in this patent specification, where dimensions of thecross-section in the direction of light propagation are typically a fewmicrons as compared to tens of microns for known surface illuminatedphotodiodes or avalanche photodiodes. Known waveguide PD/APO are oftenonly single mode optical systems whereas surface illuminated PD/APOdescribed in this patent specification can be used in both single andmultimode optical systems. In addition, known waveguide photodiodes aredifficult to test at wafer level, whereas surface illuminatedphotodiodes described in this patent specification can be easily testedat wafer level. Known waveguide photodiodes/avalanche photodiodes areused mostly in specialty photonic circuits and in many cases requirecareful temperature control, which can be costly and inefficient in ahostile data center environment. A top or bottom illuminated Si and Geon Si or GeSi on Si PD/APO that can be integrated with Si is not knownto the inventors herein to be commercially available at data rates of 25Gb/s or more at wavelengths of 850-950 nm, 1250-1350 nm and 1550-1650nm. In contrast, photodiodes on Si based material, as described in thispatent specification, can be monolithically integrated with integratedelectronic circuits on a single Si chip, thereby significantly reducingthe cost of packaging. In addition, the microstructured PD/APO at 850nm, 1300 nm and 1550 nm nominal wavelengths described in this patentspecification can be predominantly for short haul (short reach), mediumhaul (reach gap) and long haul (long reach), distances less than 300meters, in certain cases less than 2000 meters, in certain cases lessthan 10000 meters and in certain cases greater than 10000 meters opticaldata transmission. The microstructured PD/APO direction of incidentoptical beam and the electric field in the “I” region of a PIN or NIPstructure, can be predominately collinear and/or almost collinear. Inlateral PDs and APDs described in this patent specification, theelectric field and light propagation can be in different direction, butthe absorption layer can still be much thinner than in devices known tothe inventors herein for comparable data rate and/or absorption andquantum efficiency. This patent specification enables such a device andis expected to transform the current data centers to almost all opticaldata transmission between blades, within a blade, between racks and/orbetween data centers, that will vastly increase the data transmissionbandwidth capabilities and significantly reduce electrical power usageand at the same time improve performance of the monolithicallyintegrated photodetector array with microstructure holes to enhanceoptical absorption and therefore the external quantum efficiency toCMOS/BiCMOS application specific integrated circuits due to lowerparasitics such as capacitance, inductance and resistance. Thephotodetectors can be photodiodes, avalanche photodiodes, and/or singlephoton avalanche photodiode (SPAD).

In addition to data communication applications, the fast and efficientmicrostructure hole photodetectors can be used in time of flightapplications such as light direction and ranging (LiDAR), 30 imaging inthe near infrared wavelength regions. Monolithic integration ofelectronics and microstructured hole photodetectors with or without gaincan improve performance and reduce cost. The market size is in the multibillion dollars per year range.

The subject matter claimed herein is not limited to embodiments thatsolve any specific disadvantages or that operate only in environmentssuch as those described above. Rather, this background is only providedto illustrate one exemplary technology area where some embodimentsdescribed herein may be practiced.

Each published document referenced in this patent specification ishereby incorporated by reference.

SUMMARY

According to some embodiments, an integrated, single-chip structurecomprises a photosensitive portion at one side of a substrate and anactive CMOS or BICMOS electronic circuit at an opposite side of thesubstrate, wherein: said photosensitive portion at one side of saidsubstrate comprises at least one photodetector comprising a P-dopedregion, an N-doped region, and an I-region of low doped or undopedsemiconductor material that is between the N-doped region and theP-doped region and has at least one hole deliberately formed to extendinto said photosensitive portion; said I-region is essentiallysingle-crystal semiconductor material having inherent crystal planes andsaid at least one hole extents into said photosensitive portion to adepth exceeding a depth of an inverted pyramid hole with sides alongsaid crystal planes; said active circuit at an opposite side of saidsubstrate comprises plural active electronic elements; connectingelectrodes are configured to carry to said active electronic circuitelectrical signals generated by said photosensitive portion in responseto illumination, for processing by said active electronic circuit; andoutput electrodes are connected to said active electronic circuit andare configured to deliver electrical signals processed by the activeelectronic circuit.

Said P-doped region, N-doped region, and I-region can be verticallyarranged to form a vertical device or can be laterally arranged to forma lateral device.

In the vertical device configuration, in which said regions arevertically arranged, the structure can include one or more of thefollowing features: said at least one hole can extend through one andtoward the other of said P-doped region and N-doped region; material ofone of said P-doped region and N-doped region can be included atsidewall portions of said at least one hole; said I-region can be at aclosed end of said at least one hole and along at least sidewallportions thereof; one of said P-doped region and N-doped region canextend along at least sidewall portions of said at least one hole; saidat least one hole can extends through said P-doped region and N-dopedregion; said at least one hole can comprises plural holes laterallyspaced from each other and said photosensitive portion can compriseplural photodetectors; at least one avalanche photodiode structure canbe included in the photosensitive portion; and at least one singlephoton avalanche photodiode (SPAD) can be included in the photosensitiveportion.

In the lateral configuration, in which said P-doped region, N-dopedregion, and I-region are laterally arranged, the structure can includeone or more of the following features: one of said P-doped region andN-doped region can be at a closed end and at sidewall portions of saidat least one hole; said at least one hole can extend through at leastone of said P-doped region and N-doped region; said at least one holecan extend into both said P-doped region and N-doped region; said atleast one hole can penetrate through both said P-doped region andN-doped region; said at least one hole can comprise plural holeslaterally spaced from each other and said photosensitive portion cancomprise plural photodetectors laterally spaced from each other; said atleast one hole can have a closed end at one of said P-doped region andN-doped region; at least one avalanche photodiode structure can beincluded in said photosensitive portion; and at least one single photonavalanche photodiode (SPAD) can be included in the photosensitiveportion.

According to some embodiments, an integrated, single-chip structurecomprises: I-regions of low-doped or undoped first semiconductormaterial that are laterally spaced from each other by deliberatelyformed first holes extending in said first semiconductor material;regions of said first semiconductor material doped to one polarity; andregions of a second semiconductor material that is different from saidfirst semiconductor material and comprise triplets each formed of aregion that is doped to an opposite polarity and is laterally betweenregions doped to said one polarity; wherein adjacent regions of saidfirst semiconductor material are laterally spaced from each other bysaid triplets of the second semiconductor material; wherein saidI-regions and regions of said first semiconductor material doped to saidone polarity and said regions of said second semiconductor materialdoped to an opposite polarity are configured as photodetectorsgenerating electrical signals in response to illumination, whereillumination concurrently illuminating plural ones of said holescontributes to a respective single one of said electrical signal; andwherein said regions of said second semiconductor material areconfigured as avalanche structures. The structure can further includefirst and second interdigitated electrodes respectively coupled to saidregions of the first semiconductor doped to said one polarity and tosaid regions of the second semiconductor material doped to said otherpolarity. Said regions of the first semiconductor doped to said oneconductivity can be spaced vertically from said regions of the secondsemiconductor material. The structure can further include additionaldeliberately formed holes in said first semiconductor material that arelaterally between adjacent ones of said first holes.

According to some embodiments, an integrated, single-chip structurecomprises: an I-region of low-doped or undoped Si semiconductormaterial; P-doped regions and N-doped regions extending in saidsemiconductor material; deliberately formed holes extending into saidsemiconductor material and laterally spacing said doped regions; whereineach P-doped region is laterally spaced from an adjacent N-doped regionby at least one of said holes; and first and second interdigitatedelectrodes, respectively coupled to said P-doped regions to said N-dopedregions; wherein said structure is configured to generate an electricalsignal in response to light concurrently impinging on a plurality ofsaid holes to generate a respective common electrical outputrepresenting said light and to operate at Gigahertz data rates.

According to some embodiments, an integrated, single-chip structurecomprises: a first I-region of low-doped or undoped Ge or Ge/Si alloysemiconductor material; a second I-region of low-doped or undoped Sisemiconductor material; doped regions in said Ge or Ge/Si material thatare doped to one polarity; doped regions in said Si semiconductormaterial that are doped to opposite polarity and laterally space fromeach other said regions doped to said one polarity; holes deliberatelyformed in said Ge or GeSi alloy material; and first and secondinterdigitated electrodes coupled respectively to said P-doped regionsand to said N-doped regions; wherein said structure is configured togenerate electrical signals in response to light and to operate atGigahertz data rates.

According to some embodiments, an integrated, single-chip structurecomprises: an I-region of low-doped or undoped Ge or GeSi alloysemiconductor material; P-doped regions and N-doped regions extending insaid semiconductor material; deliberately formed holes extending intosaid semiconductor material and laterally spacing said doped regionsfrom each other; wherein each P-doped region is laterally spaced from anadjacent N-doped region by at least one of said holes; a low-doped Siregion extending along said Ge or GeSi region at a side thereof oppositesaid doped regions; and first and second interdigitated electrodescoupled respectively to said regions doped to one conductivity and tosaid regions doped to opposite conductivity; wherein said structure isconfigured to generate electrical signals in response to light and tooperate at Gigahertz data rates

According to some embodiments, an integrated, single-chip structurecomprises: I-regions of Si semiconductor that are low-doped or undoped;first regions of said Si semiconductor material doped to one polarity;and second regions of said Si semiconductor material doped to oppositepolarity and third regions of said Si semiconductor material doped tosaid one polarity, said second a third regions forming triplets eachcomprising one of said second regions doped to opposite polarity andlocated laterally between two of said second regions doped to said onepolarity; wherein adjacent ones of said first regions are laterallyspaced from each other by at least one or said triplets; deliberatelyformed holes extending into said I-regions, wherein a plurality of saidholes is laterally between each adjacent pair of one of said firstregions and one of said triplets; wherein said !-regions and said secondregions are configured as photodetectors generating electrical signalsin response to illumination, and said triplets are configured asavalanche structures.

According to some embodiments, an integrated, single-chip structurecomprises a photosensitive portion at one side of a substrate and anactive CMOS or BICMOS electronic circuit that is at an opposite side ofthe substrate, wherein: said photosensitive portion at one side or ofsaid substrate comprises plural sets of regions, each set comprising aP-doped region, an N-doped region, and an I-region of low doped orundoped semiconductor material that is between the N-doped region andthe P-doped region; plural holes extend in said photosensitive regionsand are laterally located between said sets; said active circuit at anopposite side of said substrate comprises plural active electronicelements; first and second electrodes connect respectively said P-dopedregions and said N-doped regions and are configured to carry electricalsignals generated by said photosensitive portion in response toillumination to said active electronic circuit for processing; whereinat least two of said sets are connected to combine the electricalsignals they generate into a common signal; and output electrodes areconnected to said active electronic circuit and are configured todeliver electrical signals processed by the active electronic circuit.Each of said sets can comprise a vertical stack of regions or,alternatively, the regions of each of said sets can be laterally spacedfrom each other. Said holes are arranged in an aperiodic array.

The term “hole” refers in this patent specification to a deliberatelyformed volume of material shaped and dimensions as specified, thatdiffers from surrounding material in specified electrical and/or opticalproperties. The material of a hole can be solid, such as a semiconductorwith such different electrical/optical properties, or a dielectric, or agas such as air, or even vacuum. A hole can be into a top surface of alayer, or into a bottom surface, or can be an internal volume that isbetween a top layer and a bottom layer of a device. Numerous examples ofsuch holes are described in detail infra., and some are interchangeablycalled protrusions, for example when a hole in the underside of anI-layer is an indentation filled with material protruding from a layerbelow.

The term “electrode” refers in this specification to material thatserves to create desired electrical fields in the disclosed devices andto extract desired electrical signals that the devices produce inresponse to light illumination. Numerous examples of electrodes aredescribed in detail infra., for example electrodes that compriseelectrically conductive material in ohmic contact with doped regions ofa device, or electrically conductive material that makes other types ofcontact such as Schottky junctions.

The terms “top” and “bottom” and similar terms refer to a specifiedorientation of a device so that, for example, the top of a device beingdescribed below becomes its bottom when the device is flipped over orbecomes its left or right side when the device is turned 90 degrees.

BRIEF DESCRIPTION OF THE DRAWINGS

To further clarify the above and other advantages and features of thesubject matter of this patent specification, specific examples ofembodiments thereof are illustrated in the appended drawings. It shouldbe appreciated that these drawings depict only illustrative embodimentsand are therefore not to be considered limiting of the scope of thispatent specification or the appended claims. The subject matter hereofwill be described and explained with additional specificity and detailthrough the use of the accompanying drawings in which:

FIG. 1. is a schematic cross-section view of an interdigitatedmetal-semiconductor-metal (MSM) Ge/GeSi photodetector;

FIGS. 2A-2F are schematic views of a vertical N-I-P Ge/GeSi photodiodewith microstructure holes on SOI monolithically integrated withCMOS/BiCMOS ASICs, according to some embodiments;

FIG. 3A is a schematic cross-section of Ge and/or GeSi on Si lateralinterdigitated avalanche photodiode (APO), according to someembodiments;

FIG. 3B is a schematic cross-section of a lateral avalanche photodiode(APO) or single photon avalanche photodiode (SPAD), according to someembodiments;

FIG. 4A is a schematic cross-section of a lateral interdigitated Ge orGe/GeSi on Si APO where optical absorption occurs in the Ge, andmultiplication occurs in Si, according to some embodiments;

FIG. 4B is a schematic cross-section of a structure similar to FIG. 4Awith the addition of microstructure holes 412 in the Ge/GeSi layer,according to some embodiments;

FIG. 5A is a schematic cross-section of interdigitated Ge/GeSi on Siphotodiode with an interdigitated Ge/GeSi on Si APD/SPAD on a singlechip, according to some embodiments;

FIG. 5B is a schematic cross-section of lateral photodiode together witha lateral APD/SPAD similar to FIG. 5A with the addition ofmicrostructure holes to enhance absorption and therefore the externalquantum efficiency (EOE), according to some embodiments;

FIG. 6 is a simple 30 perspective view of a chip where thephotodetectors are monolithically integrated with CMOS/BiCMOS ASICselectronics and lasers, according to some embodiments;

FIG. 7A is a schematic top view of a surface emitting laser, accordingto some embodiments;

FIG. 7B is a partial side view schematic drawing of a surface emittinglaser chip with tabs on its top surface;

FIGS. 8A-8E are cross-sections of photodiodes according to someembodiments;

FIG. 9. is a simplified partial top view drawing of a single chip withdetector and laser arrays, and where the detectors are monolithicallyintegrated with CMOS/BiCMOS electronics, according to some embodiments;

FIG. 10. is a simplified partial schematic top view drawing of a chipwith lasers and 20 array of microstructure hole photodetectors that canbe used for 3D imaging in LiDAR systems, according to some embodiments;

FIGS. 11A-B are partial simplified cross-section schematics of lateralphotodetectors;

FIG. 12 is a partial cross-section of a lateral Si avalanchephotodiode/single photon avalanche photodiode with P and N junctions,according to some embodiments;

FIGS. 13A-B show laser pulses that can have a certain sequence of pulsesfor LiDAR applications in order to distinguish between different LiDARsignals that may exist in the same environment;

FIGS. 14A-C show experimental results for vertical PIN microstructurehole photodetector;

FIGS. 15A-B are plots showing experimental current-voltage (IV)characteristics of lateral Si MSM contacts with and without nativeoxide, according to some embodiments;

FIGS. 16A-16D are experimental gain plots of an Si microstructure holePIN photodiode in a vertical configuration;

FIGS. 17A-17H are plots of shows FDTD (finite difference time domain)simulation of the optical field of various microstructure holestructures, according to some embodiments;

FIGS. 18A-B are simplified partial cross-sections of a lateralinterdigitated photodetector with metal oxide semiconductor (MOS)junctions, according to some embodiments;

FIG. 19 is a simplified partial cross-section of an interdigitatedlateral photodetector, according to some embodiments;

FIGS. 20A-D are schematics a LiDAR and/or camera system wherein detectorarrays are monolithically integrated with CMOS/BiCMOS ASICs on one ormore chips, according to some embodiments;

FIGS. 21A-21C are simplified partial schematic cross-sections of alateral APO/SPAD Ge/GeSi on Si where the absorption of the opticalsignal are predominately in the Ge/GeSi and the multiplication such asavalanche gain occurs in the Si, according tq, some embodiments;

FIG. 22A shows a simplistic cross-section schematic of a interdigitatedvertical Ge/GeSi on Si APO/SPAD with or without BOX layer, according tosome embodiments;

FIG. 22B shows a simple top view of the structure shown in FIG. 22Awhere the interdigit anodes and cathodes are connected to a transmissionline and can be monolithically integrated with CMOS/BiCMOS ASICs,according to some embodiments;

FIGS. 23A-B, 24A-B, 25A-B and 26A-B are schematic cross-sections ofinterdigitated lateral Ge/GeSi on Si APDs/SPADs, according to someembodiments;

FIGS. 27A-B show a schematic cross-section and top view of Ge strips onSi with and without microstructure holes for use in FDTD simulation ofoptical absorption in the Ge strips;

FIG. 28 shows a FDTD simulation of absorption of Ge strips on Si withoutmicrostructure holes vs wavelength from 1-1.6 microns;

FIG. 29 shows FDTD simulation of optical absorption in Ge strips on Siwith microstructure holes vs wavelength from 1-1.6 microns;

FIGS. 30A-B are simplified partial schematic top views of asemiconductor surface having holes configured as trenches, according tosome embodiments;

FIGS. 31A-B shows simplified partial cross-section schematics of a SPADor APO or PD Si photodetector for imaging and LiDAR applications,according to some embodiments;

FIGS. 32A-B shows partial simplified cross-section schematics similar toFIG. 31B with the addition of a Ge/GeSi layer on top of the N well,according to some embodiments;

FIGS. 33A-C show simplified partial schematic cross-sections ofmicrostructure holes formed on semiconductor surfaces, according to someembodiments;

FIGS. 34A and 35A show known optical modules;

FIGS. 34B and 35B show optical modules, according some embodiments;

FIGS. 36A-B show simplified partial schematic top views of aninterdigitated photodiode and elongated microstructure holes, accordingto some embodiments;

FIG. 37 shows current voltage characteristics “IV” of a metal oxidesemiconductor junction under both M1 and M2 electrodes of aninterdigitated photodiode, according to some embodiments;

FIGS. 38A-C illustrate an FDTD simulation of a structure, according tosome embodiments;

FIGS. 39A-C show partial simplified cross-section schematics ofinterdigitated Ge/GeSi on Si photodiode, according to some embodiments;

FIG. 39D shows a simplified cross-section of Ge on Si pyramids used forFDTD simulation;

FIG. 39E shows the FDTD simulation of the structure shown in FIG. 39D;

FIG. 40 shows a simplified partial cross-section of a monolithicintegrated Photodetector array with CMOS/BiCMOS ASICs, according to someembodiments;

FIGS. 41A-C show simplified views of pits etched on a Si surfaceconfigured for fluidic self-assembly, according to some embodiments;

FIGS. 42A-B and 43A-B are partial simplified cross-sections of a Ge/GeSion Si photodiode, according to some embodiments;

FIGS. 44A-D, 45A-C and 46A-D show basic simplified steps for monolithicintegration of microstructure holes photodetector with CMOS and/orBiCMOS ASICs, according to some embodiments;

FIGS. 47A-C and 48A-C show a basic simplified processing steps tomonolithically integrate interdigitated photodetector with CMOS/BiCMOSASICs, according to some embodiments;

FIGS. 49A-F show basic fabrication steps for Ge/GeSi on Siinterdigitated photodiode that can be monolithically integrated withCMOS/BiCMOS ASICs, according to some embodiments;

FIG. 50 shows a simplified partial cross-section schematic of a Ge/GeSion Si photodiode that can be monolithically integrated with CMOS/BiCMOSASICs, according to some embodiments;

FIGS. 51A-D show simplified partial cross-section schematic examples ofmicrostructure holes where microstructure holes can be defined asregions where the optical refractive index is lower than in thesurrounding material, according to some embodiments;

FIG. 52 shows a simplified partial cross-section schematic of aninterdigitated Ge on Si SOI photodiode with lateral P and N wells withmicrostructure holes between the interdigits, according to someembodiments;

FIG. 53A shows a simplified 3D schematic of a Ge on Si SOI lateral PINinterdigitated photodetector, according to some embodiments;

FIG. 53B shows a simplified 30 schematic of an interdigitated lateralPIN photodetector with interdigitated electrodes such as shown in FIG.52;

FIGS. 54A-C show FDTD simulated optical absorption of a structure suchas shown in FIG. 52;

FIG. 55 shows experimental data of external quantum efficiency vs.reverse bias voltage of an interdigitated MSM photodetector on SOI wherethe device layer is 1 micron thick;

FIGS. 56A-D show the impulse responses at 850 nm wavelength of a devicewith EOE shown in FIG. 55;

FIGS. 57-59 shows simple partial cross-section of a bottom illuminatedCMOS/BiCMOS sensor array, according to some embodiments;

FIGS. 60A and 60B show a cross-section view and bottom view,respectively, of a microstructure hole back illuminated CMOS/BiCMOSsensor array, according to some embodiments;

FIGS. 61 and 62 are simplified partial cross-sections of amicrostructure hole bottom illuminated CMOS/BiCMOS sensor array,according to some embodiments;

FIGS. 63A-B show a simplified partial bottom schematic views of a backilluminated CMOS/BiCMOS sensor array with circular holes, according tosome embodiments;

FIG. 64 is a diagram illustrating hexagonal holes in a hexagonallattice, according to some embodiments;

FIG. 65 shows a FDTD simulated optical absorption vs wavelength for a 1micron device layer on SOI with microstructure holes diameter of 1000 nmand 1300 nm period in a square lattice;

FIG. 66 shows a FDTD simulation of a 0.5 micron Si device layer on SOIstructure;

FIGS. 67A-B are linear and semi-log plots, respectively, of the IVcharacteristics with and without 850 nm wavelength illumination;

FIGS. 68A-D and 69A-D show impulse responses and eye diagrams of aninterdigitated Si MSM with microstructure holes, according to someembodiments;

FIG. 70 shows the percentage of the capacitance change of a PIN/NIPvertical structure photodetector with and without microstructure holes;

FIG. 71 shows FDTD simulated optical absorption in Si layers on SOI. TheSi device layer range from 1000 nm-200 nm as shown in the plots;

FIGS. 72A-B show simplified partial cross-sections of a Si MSM,according to some embodiments;

FIG. 73 shows a simplified partial schematic of a top view of the devicedepicted in FIGS. 72A-B;

FIG. 74A-B shows cross-section schematics of Ge and/orGeSi selectivearea grown on regions where there is Si, according to some embodiments;

FIG. 75A shows a top view of the device shown in FIG. 74A;

FIG. 76 shows a simplified top view of a device such as shown in FIG.74A;

FIGS. 77A-B show a simplified partial cross-section and top viewrespectively of Si dioxide/dielectric deposited on a Si surface andwhere holes configured as slots form a pattern such as a cross-hatch,according to some embodiments;

FIGS. 78A-B, 79A-B and 80 show simplified partial cross-sections and topviews of selective area epitaxial growth of Ge and/or GeSi on Si andwhere the surface can be planarized using CNP for example, according tosome embodiments;

FIGS. 81A-D show simplified partial schematic cross-sections of aninterdigitated Si photodiode on SOI wafer, according to someembodiments;

FIGS. 82A-C show simple partial cross-sections and top views of Silateral PIN photodetectors with microstructure holes formed, accordingto some embodiments;

FIGS. 83A-C and 84A-C show FDTD simulations of optical absorption ofmicrostructure holes on SOI wafer, according to some embodiments;

FIGS. 85A-B show partial simplified cross-sections of microstructureholes on a thin Si device layer, according to some embodiments;

FIG. 86A shows a cross-section schematic of a microstructure holephotodetector, according to some embodiments;

FIG. 86B shows a cross-section schematic of a Ge/GeSi on Simicrostructure hole photodetector, according to some embodiments;

FIG. 86C shows a Si microstructure hole vertical PIN where theinterdigits are anodes and the cathode electrode can be formed on the N+Si, according to some embodiments;

FIG. 87 is a schematic top view of a vertical PIN photodetector,according to some embodiments;

FIGS. 88A-C show an FDTD simulation of the optical field impinging onthe top device layer surface;

FIGS. 89A-B show an FDTD simulation of a microstructure hole structure;

FIGS. 90A-B show an FDTD simulation of the optical field of amicrostructure hole structure;

FIGS. 91A-B show an FDTD simulation of the optical field of amicrostructure configuration;

FIGS. 92-94 show partial cross-section schematics of lateral PINinterdigitated photodiodes, according to some embodiments;

FIG. 95 shows a simplified partial cross-section schematic of a bottomilluminated CMOS image sensor or a bottom illuminated CMOS high speedvertical PIN photodiode, according to some embodiments;

FIG. 96 shows a simplified partial cross-section schematic of a bottomilluminated CMOS image sensor or a bottom illuminated CMOS high speedvertical PIN photodiode, according to some embodiments;

FIGS. 97A-B and 98A-B are partial schematic cross-sections similar toFIGS. 95 and 96;

FIGS. 99A-B show an FDTD simulation of optical fields that are absorbedin an thin SI layer on top of a BOX layer in a SOI structure.

FIGS. 100A-B are partial schematic cross-sections of structure similarto that shown in FIG. 99A;

FIGS. 101A-B show an FDTD simulation of surface illuminated opticalfield of a structure, according to some embodiments;

FIGS. 102A-B and 103A-C show FDTD simulations of surface illuminatedoptical field of a structures;

FIGS. 104A-G are a simplified partial schematic of a top views ofphotodetector arrays configured as dense 2D arrays for imagingapplications, according to some embodiments;

FIGS. 105A-C shows simplified partial cross-sections of a singlemicrostructure hole in a pixel, according to some embodiments;

FIG. 106 shows experimental results of absorption enhancement withmicrostructure holes or microholes;

FIGS. 107A-C shows simplified partial schematic of a top views and across-section of a pixel with a single microstructure hole, according tosome embodiments;

FIGS. 108A-C show an FDTD simulation of a thin Si device layer on SOIsubstrate where the Si is 30 nm thick, the BOX layer is 100 nm on Sisubstrate;

FIG. 109 shows a partial schematic cross-section of a light trappingstructure, according to some embodiments; and

FIGS. 110A-C show FDTD simulated optical absorption, reflection andtransmission of a single hole pixel in Si on a BOX layer, according tosome embodiments.

DETAILED DESCRIPTION

A detailed description of examples of preferred embodiments is providedbelow. While several embodiments are described, it should be understoodthat the new subject matter described in this patent specification isnot limited to any one embodiment or combination of embodimentsdescribed herein, but instead encompasses numerous alternatives,modifications, and equivalents. In addition, while numerous specificdetails are set forth in the following description in order to provide athorough understanding, some embodiments can be practiced without someor all of these details. Moreover, for the purpose of clarity, certaintechnical material that is known in the related art has not beendescribed in detail in order to avoid unnecessarily obscuring the newsubject matter described herein. It should be clear that individualfeatures of one or several of the specific embodiments described hereincan be used in combination with features or other described embodiments.Further, like reference numbers and designations in the various drawingsindicate like elements.

All publications cited in this patent specification are herebyincorporated by reference. Some of the figures described herein aresimplified in that for clarity they may omit elements of structures thatskilled persons would understand need not be shown expressly and thefigures may show only a portion of a structure that comprises repeatedpatterns of the shown portions. For example, a figure may show a devicewith a single pair of laterally spaced electrodes where the actualdevice being described includes a collection of two or more such regionson or in the same substrate. The Greek letters v (nu) and TT (pi) denotein this specification semiconductor material that is low doped to N andP doping, respectively, e.g., to no more that about 10¹² per cm³ doping.The semiconductor material regions described in this patentspecification are material that is single-crystal or essentiallysingle-crystal except for the deliberately formed “holes” describedbelow, unless otherwise specified. The terms “partial” or “partially”regarding the depth of holes or or of etching refer in thisspecification to holes that extend partway into a region rather thanthrough the entire region.

FIG. 1. is a schematic cross-section view of an interdigitatedmetal-semiconductor-metal (MSM) of Ge/GeSi photodetector. The Ge/GeSilayer is formed on Si and an insulator (SOI). The Si device layer is Ior low dope P type with resistivity greater than or equal to 5 ohm/cmand with a thickness ranging from 100-1000 nanometers approximately. AGe/GeSi layer is selective area grown on the Si device layer with orwithout a low temperature Ge/GeSi buffer layer(s) and where the Ge/GeSilayer is I or low dope and with a thickness ranging from 100-1000 nm,and in some cases 200-700 nm, and in some cases 300-500 nm. A thin Aloxide layer can be deposited on the Ge/GeSi with thickness ranging from1-10 nm to reduce leakage current. Metal and/or metal silicide form theinterdigits of electrodes M1 and M2. Microstructure holes 112 and 114are dry etched into the Ge/GeSi layer fully or partially. In some casesthe etch can extend to the bottom of the Ge/GeSi layer as in hole 114.In some cases a wet etch can be performed after the dry etch in Si toform inverted pyramids, as in hole 112. The lateral dimension of themicrostructure hole can range from 500-1700 nm or more, and the spacingbetween the microstructure holes can range from 100-300 nm or more. Theshape of the microstructure holes can be circular, rectangular,polygonal, inverted pyramids, and/or any combination of shapes. Themicrostructure holes can be a in a square or hexagonal lattice, and canbe periodic, and/or aperiodic. The interdigit electrode spacing canrange from 500-1000 nm or more, and in some cases can range from 300 to1000 nm or more. The width of the interdigit electrodes can range from30 to 300 nm or more. The length of the interdigits can range from 5microns to 100 microns or more, and in some cases 10-50 microns.

The microstructure holes can be not filled, partially filled, or fullyfilled with dielectric or poly crystalline semiconductor. In some casesthe Al oxide layer can be replaced with I or low dope Poly Si, withthickness ranging from 10-300 nm or more. The interdigitatedphotodetector, is monolithically integrated to CMOS/BiCMOS applicationspecific integrated circuits (ASICs). Not shown are transmission linesconnecting the interdigits M1 and M2 to the CMOS/BiCMOS electronics.

In some cases the interdigits M1 and M2 can be formed partially into theGe layer. And in some cases P and N wells can be formed beneath M1 andM2 to form a P-1-N junction between M1 and M2. In the case of P-1-N areverse bias is applied between M1 and M2 where the Pis more negativethan the N. In the case where M1 and M2 are Schottky contacts or metaloxide semiconductor contacts the interdigitated detector can be operatedin both the forward or reverse voltage bias.

Wavelength can range from 800 nm to 1800 nm and in some cases from 800nm-1600 nm, in some cases from 1000 nm to 1400 nm and in some cases700-2200 nm.

Reverse bias voltage for P-I-N can range from 1 to 10 volts or more, andbias voltage for Schottky contacts that can be symmetric in both theforward and reverse bias can range from 1 to 10 volts or more. In somecases at voltages of 10 volts or more gain can be observed in theexternal quantum efficiency that can be due to avalanche gain forexample. In some cases gain can be observed at less than 10 volts.Optical signal can impinge from the top surface where the interdigitsare or on the bottom substrate surface. Not shown are passivationantireflection layers. In some cases the microstructure holes can beetched partially into the Ge/GeSi layer, and in some cases it can beetched partially into the Si layer, and in some cases it can be etchedto the BOX layer. In some cases the microstructure holes can be etchedinto the BOX layer, and in some cases through the BOX layer.

The lateral dimension of microstructure holes in most cases mentioned inthis patent specification are for microstructure holes not filled withany dielectric, and filled only with air or vacuum where the opticalrefractive index is approximately 1. In the cases where themicrostructure holes are filled fully or partially with the dielectriclateral dimension of the microstructure hole can be reduced by theeffective optical refractive index of the dielectric/voids in themicrostructure holes. For example a microstructure hole with lateraldimension of 800 nm when not filled in air can have a lateral dimensionof 533 nm if completely filled with SiO2 which has an optical refractiveindex of approximately 1.5. The microstructure hole lateral dimensioncan in some cases be reduced when filled with dialectic, where therefractive index is greater than 1 for example (lateral dimension ofmicrostructure hole in vacuum or air)/(optical refractive index), and insome cases where the microstructure hole is partially filled withdielectric and effective optical refractive index can be calculated bythe ratio of the volume of 1 or more dielectrics in the microstructurehole.

FIGS. 2A-2F are schematic views of a vertical N-I-P Ge/GeSi photodiodewith microstructure holes on SOI monolithically integrated withCMOS/BiCMOS ASICs, according to some embodiments.

FIG. 2A. is a cross-section of a SOI wafer with a P+ region 208 that canbe doped by diffusion or I implantation of Boron ions in selectiveareas, for example beneath the photodetector. This formation of P+ wellcan be part of the CMOS/BiCMOS process.

FIG. 2B. shows Ge/GeSi selective area grown over the P+ well region withGe/GeSi layer that can be I or low doped and with thickness ranging from200-1000 nm, and in some cases 300-500 nm. The Ge/GeSi layer can includea buffer layer between the Ge/GeSi and the Si device layer. The N+ polySi layer can be deposited on the Ge/GeSi layer, with a thickness rangingfrom 100 nm to 1000 nm and in some cases 100 nm-500 nm. A transparentconducting metal oxide can be deposited on the N or N+ poly Si to reducethe series resistance. In some cases multiple cathodes can be formed onthe N poly Si. Anode can be formed on the P+Si. Microstructure holes areetched in the poly Si, and in some cases can extend into the Ge/GeSi,and in some cases can extend through the Ge/GeSi layer. Themicrostructure holes 212 can be unfilled, partially filled, or fullyfilled with dielectric and/or poly semiconductor. The dimension of themicrostructure holes can be similar to that of FIG. 1.

FIG. 2C shows selective area grown Ge/GeSi on SOI such as in FIG. 2Awith microstructure holes 212 formed by selective area growth with SiO2islands. The SiO2 islands can have similar lateral dimensions andspacing as the holes described in FIG. 1, and the thickness of the SiO2islands can range from nm-500 nm or more. N poly Si can be formed on thesurface of the Ge/GeSi and in some cases can be formed on the sidewallsof the microstructure holes. The N poly Si can have a thickness rangingfrom 100 to 500 nm, in some cases a transparent conducting metal oxidecan be formed on the surface of the poly Si. Cathodes are formed on theN poly Si, and anodes formed on the P+Si.

FIG. 2D. is similar to FIG. 2C except that the N poly Si is only on thetop surface of the Ge, and not in the holes. In some cases, the poly Sican be partially in the microstructure holes. The microstructure holescan be unfilled, partially filled, or fully filled with dielectricand/or poly semiconductor.

FIG. 2E. is a schematic top view of the microstructure hole photodiodeof FIGS. 2B, 2C and 2D showing a region 250 of selective area grownGe/GeSi and in some cases can be etched mesa where the cathode ring 222is formed on the selective area growth and/or mesa of the Ge/GeSi layer250 and the anode 220 is formed on the P+ Si. Microstructure holes 212are shown that can be etched or formed by selective area growth. Theholes can be unfilled, partially filled, or fully filled with dielectricand/or poly/amorphous semiconductor. The photodiode or arrays ofphotodiode can be monolithically integrated with CMOS/BiCMOS ASICs. Notshown are transmission lines connecting the photodiode to theCMOS/BiCMOS electronics. Also not shown are isolation trenches, lightshields, passivations, anti-reflections to name a few.

FIG. 2F is another top view that shows an addition of vertical and/orhorizontal metal/metal silicide electrodes 224 connecting to the cathode222. In some cases, the metal/metal silicide can be a grid as shown. Thegrid can allow a more uniform distribution of the electric field incases where the N poly Si conductivity is low. For example, where the Npoly Si has sheet resistance of 100 ohm per square or more. The width ofthe metal and/or metal silicide electrodes can range from 20 nm-300 nm.Anti-reflection coating and/or nanostructures of amorphoussemiconductors can be deposited on the metal electrode to reducereflection. In some cases, transparent metal conducting oxide can bedeposited on the surface of the poly Si to reduce the series resistance.

The horizontal and/or vertical electrodes connected to the cathodeillustrated in FIGS. 2A-F can be spaced by 1 or more hole spacing, andin some cases with both vertical and horizontal electrodes such as in agrid pattern, the spacing of the electrodes can be by 1 or more holes.In some cases, the electrodes connecting to the cathode can bemeandering and not necessarily straight lines. This example is for aN-1-P structure, and the N and P can be interchanged, in which case thecathode is replaced by the anode, and the anode is replaced by thecathode.

FIG. 3A is a schematic cross-section of Ge and/or GeSi on Si lateralinterdigitated avalanche photodiode (APO), according to someembodiments. The photodiode can be and APO and/or single photonavalanche photodiode (SPAD) with a lateral P, I or low dope PNstructure. A reverse bias is applied between the electrodes M1 and M2.In some cases, the lateral APD/SPAD can be a P, I or low dope Nstructure. The Ge, and/or GeSi layer thickness can range from 100 nm to1000 nm or more, and in some cases 300 nm to 700 nm. A low temperatureGe buffer layer can be included prior to the high temperature growth ofGe on Si. For example, see reference Dehlinger et al, High-SpeedGermanium-on-SOI Lateral PIN Photodiodes, IEEE Photonics TechnologyLetters, Vol. 16, No. 11, November 2004. These structures can bemonolithically integrated with CMOS/BiCMOS ASICs, for example seereference, Koester et al, Ge-on-SOI-Detector/Si-CMOS-Amplifier Receiversfor High-Performance Optical-Communication Applications, Journal ofLightwave Technology, Vol. 25, No. 1, January 2007. A box layer can beincluded, the Si device layer can have thickness ranging from 10 nm-1000nm or more. Light or optical signal can impinge on the top surface ofthe Ge/GeSi or from the bottom surface Si or BOX surface. Wavelength canrange from 800 nm to 1800 nm, and in some cases 800 nm-1400 nm or more,and in some cases from 800 nm-1550 nm.

A light shield can be included to shield the PNP multiplication regionover the M2 electrode for example.

FIG. 3B is a schematic cross-section of a lateral avalanche photodiode(APO) or single photon avalanche photodiode (SPAD), according to someembodiments. The APD/SPAD interdigitated photodetector is similar toFIG. 3A except with the inclusion of microstructure holes forenhancement of absorption. The microstructure holes 312 are formed inthe Ge/GeSi layer as shown and can have an etch depth ranging from 100nm to 1000 nm or more, and in some cases the microstructure holes arepartially in the Ge or etched though the Ge/GeSi to the Si layer, and insome cases into the Si layer, and in some cases through the Si layer tothe BOX layer. The microstructure holes can be unfilled or partiallyfilled, or fully filled with dielectric, and/or amorphous/polysemiconductor. The dimensions of the microstructure holes can range from400 nm to 2000 nm, and in some cases 500 nm-1500 nm. The spacing betweenadjacent holes can range from 0 nm (touching or overlapping) to 1000 nm,and in some cases, from 100 nm to 500 nm. In the case of 0 nm ortouching the holes can be conical such that the tops of the holes cantouch, but not the bottoms of the holes. The cross-sectional shape ofthe holes can be cylindrical, conical, polygonal, and any combination ofshapes. The holes can be circular, square, or polygonal, and can beaperiodic, and/or periodic, and/or random pattern.

Not shown in FIGS. 3A-B are passivation layers, CMOS/BiCMOS ASICs,anti-reflection coating, light shields, and isolation trenches to name afew.

FIG. 4A is a schematic cross-section of a lateral interdigitated Ge onSi APO where optical absorption occurs in the Ge, and multiplicationoccurs in Si, according to some embodiments. The structure can be a P(Ge/GeSi), I or low dope Ge/GeSi/Si and PN on Si. The strips of Ge underthe M1 electrode can be grown using selective area growth or the stripscan be formed by etching the Ge to the Si layer. The Ge/GeSi can be I orlow doped with thickness ranging from 100 nm-1000 nm or more, and insome cases 300 nm-700 nm. A P doped well is formed in the Ge and the M1electrode forms an ohmic contact to the P doped well. P and N wells areformed in the Si and the M2 electrode forms an ohmic contact to the Nwell. A reverse bias is applied between the M1 and M2 electrode.

Multiplication occurs in the PN junction in the Si layer and photonabsorption generating electron hole pairs occurs in the Ge/GeSi layer.For LiDAR (Light distance and ranging) applications the spacing betweenthe interdigits can range from 1 micron to 100 microns or more, and insome cases 5 microns-50 microns. The width of the Ge strip can be 50% ormore of the spacing between M1 and M2 electrodes. The width of the M1and/or M2 electrode can range from 20 nm to 300 nm or more, and thelength of the interdigitated electrode can range from microns to 100microns or more. The Si device layer can range from 10 nm to 1000 nm ormore. A BOX layer can be included. Wavelength range of the opticalsignal or light can be from 1000 nm to 1800 nm, and in some cases 800nm-1800 nm. In some cases, a light shield can be included to cover themultiplication region. Not shown are passivation layers, anti-reflectioncoating layers, CMOS/BiCMOS ASICs, transmission lines to name a few.

FIG. 4B is a schematic cross-section of a structure similar to FIG. 4Awith the addition of microstructure holes 412 in the Ge/GeSi layer,according to some embodiments. As shown, there is a singlemicrostructure hole between the M1 and M2 electrode, and in some casesthere can be multiple holes between M1 and M2 electrodes depending onthe spacing between the M1 and M2 electrodes. The hole dimensions aresimilar to those in FIG. 3B. The addition of microstructure holes 412enhances the optical absorption and can have a higher external quantumefficiency than a similar structure such as in FIG. 4a at certainwavelength ranges. Photons can impinge on the top surface or from thebottom surface of the Si substrate. A reverse bias is applied betweenthe M1 and M2 electrode with bias voltage ranging from 1 to 100 volts ormore, and in some cases 5-35 volts.

In structures such as illustrated in FIGS. 4A-B, for wavelength range of1000 nm or longer for example 1000 nm to 1800 nm and in some cases 1200nm to 1600 nm photons are predominately absorbed in the Ge/GeSi layerand multiplication such as avalanche gain occurs in the Si PN regionwhen the device is reverse biased between the anode (M1) and the cathode(M2) where the voltage or potential at M1 is more negative or lower thanthe voltage or potential at M2. The reverse bias can range from −3 voltsto −50 volts or more, and in some cases −10 volts to −45 volts. In FIGS.4A and 4B a lateral PI (or low dope) PN junction is shown, and in somecases it can be a PIPIN junction and in some cases PN junction, and insome cases Schottky junctions, and in some cases metal oxidesemiconductor junctions, and in some cases any combination of junctionscan be used. A lateral separate absorption multiplication APO/SPAD(single photon avalanche diode) is shown in FIGS. 4A and 4B. A verticalseparate absorption multiplication APO is shown in Ref. Zaoui et. al,Origin of the Gain-Bandwidth-Product Enhancement inSeparate-Absorption-Charge-Multiplication Ge/Si Avalanche Photodiodes.OSA/OFC/NFOEC 2009.

FIG. SA is a schematic cross-section of interdigitated Ge/GeSi on Siphotodiode with an interdigitated Ge/GeSi on Si APD/SPAD on a singlechip, according to some embodiments. Multiple photodiodes and APO/SPADcan be fabricated on a single Si chip integrated with CMOS/BiCMOS ASICs.In some cases, photodiodes and/or APD/SPAD can have different speed ordata rate bandwidths by having different spacing between the interdigitelectrodes which can change the transit time and the RC time of thephotodetector. 2D arrays of photodiodes and APD/SPAD can bemonolithically integrated with CMOS/BiCMOS ASICs electronics on a singlechip, and in some cases Vertical Cavity Surface Emitting Lasers (VCSELs)and/or edge surface emitting lasers (ESELs) can be fluidic assembled onthe same chip. Other assembly such as robotic assembly can also be used.In some cases, the photodiode and/or APD/SPAD can have a single cycle ofthe M1 and M2 and/or M3 and M4 electrodes separated by and isolationtrench 530; for example the structure can be a lateral photodiode and/orAPD/SPAD with a wide spacing between M1 and M2 and/or M3 and M4electrodes. The spacing can be 20 microns-2000 microns or more, and insome cases 100 microns-2000 microns or more. In most cases theinterdigits of the photodiode and/or APD/SPAD have multiple cycles ofinterdigits.

FIG. 5B is a schematic cross-section of lateral photodiode together witha lateral APD/SPAD similar to FIG. SA with the addition ofmicrostructure holes 512 to enhance absorption and therefore theexternal quantum efficiency (EQE), according to some embodiments.Photodetectors with microstructure holes can have a higher EQE than asimilar photodetector without microstructure holes at certain wavelengthranges. In some cases for the photodiode, the M2 can be formed on the Geand in some cases the APD/SPAD the M4 and the multiplication regions canalso be formed on the Ge.

FIG. 6 is a simplified 3D perspective view of a chip where thephotodetectors are monolithically integrated with CMOS/BiCMOS ASICselectronics and lasers, according to some embodiments. The surfaceemitting lasers, VCSELS and ESELs 610 can be assembled on the Si chip600 using techniques that can include fluidic assembly and roboticassembly to name a few. Structures 620 can be formed on the surface ofthe chip at wafer-scale levels to assist the coupling of outgoing light622 to optical fibers for optical interconnect applications, and in thecase of LiDAR applications structures 620 can be formed over the surfaceemitting lasers to direct the incoming light 624 at an angle off normalto the surface and for the photodetector structures can be formed tocollect incoming light 624 from certain angles off normal from thesurface. In some cases, the structures 620 can direct light normal tothe surface for both the laser and for the photodetector. In the casefor directing light from the laser at angles off normal micro-prisms canbe used in conjunction in some cases with a lens. Similarly, forcollecting light coming in at an off angle, micro-prisms and lens can beused for the photodetectors 612. In this way a single chip can cover awide angle for LiDAR applications. The chip can include multiple lasers610 and detectors 612 in 1 or 2D arrays. The structures 620 for guidingthe light and/or focusing the light, and/or directing the light can beformed using micro printing techniques and/or lithographic techniques.In some cases, laser ablation can be used together with lithographictechniques, and/or micro printing techniques.

For optical data communication using structures such as illustrated inFIG. 6, 1 or 2D arrays of monolithically integrated Si and/or Ge on Siphotodetectors which can be vertical or lateral in structure withCMOS/BiCMOS ASICs and where 1 or 2D arrays of surface emitting laserswhich can be vertical cavity surface emitting lasers and/or edge surfaceemitting lasers in 1 or 2 arrays can be assembled on the same Si chip asthe photodetector and CMOS/BiCMOS ASICs. The CMOS/BiCMOS ASICs areconnected to the photodetector array and a separate set of CMOS/BiCMOSASICs can be connected to the surface emitting laser array at the waferscale level using back end of the line (BEOL) processing methods. Thissingle chip for example can provide multiple channel of opticaltransmitter and multiple channel of optical receiver. In some cases, thearray of optical transmitters can be light emitting diodes. The laser orlight emitting diode arrays can be assembled in a single or multiplechips that can have the same or different wavelength, and in some casessurface emitting laser and light emitting diodes singly or in array canbe assembled on the same Si chip as the array of photodetectors that canbe singly or array. Optical bandpass filters can be formed over theoptical detectors to select different wavelengths of incoming signals ifneeded.

For LiDAR applications using structures such as illustrated in FIG. 6,arrays of laser and/or light emitting diode can be assembled for exampleusing fluidic assembly or robotic assembly on the Si chip that containsthe monolithically integrated photodetectors connected to CMOS/BiCMOSASICs for signal processing. A separate set of CMOS/BiCMOS ASICs on thesame chip can be used to drive the laser and/or LED arrays, and wherethe lasers and LEDs can be singly or in arrays. For LiDAR applicationsthe optical transmitter can be a single or multiple or stream of opticalpulses that can be coded to enhance optical detector sensitivity and/orto distinguish the optical pulses from signals emitted by other LiDARsystems. In the case of LiDAR the pulses can have repetition ratesranging from approximately 100 hertz or less to MHz, and in some casesKHz whereas for optical data communication in data center interconnectfor example optical pulse repetition or data rate range from 1 Gb/s to50 Gb/s or more and in some cases Gb/s to 50 Gb/s, and in some casesgreater than 50 Gb/s. For certain optical data communication such asautomotive or aeronautics data rate can range from 10s Mb/s to 10 Gb/sor more, and in some cases from 0.5 Gb/s to 10 Gb/s or more.

The wavelength range for optical data communication using structuressuch as illustrated in FIG. 6, can range from 800 nm to 1750 nm, and thewavelength range for LiDAR can range from 800 nm to 1600 nm.

FIG. 7A is a schematic top view of a surface emitting laser, accordingto some embodiments. In this case, a vertical cavity surface emittinglaser 702 is fluidically assembled onto a monolithic silicon chip 700,where the photodetector and the CMOS/BiCMOS ASICs are integrated. Oncethe laser 702 is fluidically assembled, heat can be applied to solderthe bottom of the laser 702 to the bottom surface of a hole that wasetched in the silicon chip 700 to receive the laser 702. The laser 702has a light emitting area 710 and one or more tabs 740 near its topsurface to prevent the laser 702 from being positioned upside down. Oncethe laser 702 is assembled onto the silicon chip, transmission lines 730and 732 from the CMOS/BiCMOS ASICs electronics such as laser driverelectronics can be attached to the anode 720 and cathode 722,respectively, of the laser 702. In some cases, a single widetransmission line can be attached to the cathode, and a single widetransmission line can be attached to the anode 720. In some cases, thetransmission line 730 can branch, for example a Y branch such that thetransmission line contacts the anode 720 at two places as shown in FIG.7A Similarly, the transmission line 732 for the cathode can also branchin a Y geometry such that it attaches at two places on the cathode 722.In case any of the tabs at the edge of the laser is in the same positionas the transmission line at least one of the branch can make contactwith the anode or cathode. The transmission lines 730 and 732 can beapplied using standard CMOS process and lithography. Multiple branchesof the transmission line to the laser ensures a successful electricalcontact to the anode and cathode.

FIG. 7B is a partial side view schematic drawing of a surface emittinglaser chip 702 with tabs 740 on its top surface such that during fluidicassembly it cannot fall into the designated hole upside down. Inaddition, solder bump 750 can be added to the bottom of the surfaceemitting laser chip to assist in attaching the chip to the Si waferafter a brief thermal cycling to melt the solder. The weight of thesolder on the bottom of the surface emitting laser chip can alsofacilitate the process of fluidic assembly or any other self-assemblymethods since the bottom of the chip in heavier.

FIGS. 8A-8C are cross-sections of photodiodes according to someembodiments. The photodiodes shown in FIGS. 8A-8C share similarcharacteristics in terms of interdigit electrode spacing, holedimensions, data rate and bandwidth.

FIG. 8A is a schematic cross-section of a silicon interdigitatedphotodiode with microstructure holes between the interdigits. A P wellcan be formed under interdigit M1 for example, and a N well can beformed under interdigit M2. The depth of the P and N wells can rangefrom 10 nm-1000 nm or more, and in some cases approximately one half thethickness of the silicon device layer, and in some cases extending tothe BOX layer. The silicon interdigitated photodiode is fabricated on aSOI wafer (silicon on insulator) with a buried oxide (BOX) layer rangingin thickness from 10 nm-2000 nm or more, and the silicon device layercan have a thickness ranging from 300 nm-1000 nm or more, and in somecases the thickness can range from 500 nm-1000 nm, and in some cases thethickness can range from 1000 nm-5000 nm or more. The Si device layercan be undoped or low doped, and in some cases can be low P dope such asP−− (re), and in some cases the Si device layer can be N−− (re). Thespacing between the M1 and M2 can range from 300 nm or less, and in somecases the spacing between M1 and M2 can range from 300 nm-2000 nm, andin some cases the spacing between M1 and M2 electrodes can range from1000 nm-10,000 nm, and in some cases the spacing between the M1 and M2electrodes can range from 5000 nm-50,000 nm. Microstructure holes forenhancing the optical absorption and therefore the external quantumefficiency are etched into the Si with depths ranging from 300 nm-1000nm or more, and in some cases approximately halfway into the devicelayer, and in some cases to the BOX layer. The hole cross-section can bean inverted pyramid, and in some cases can be cylindrical, and in somecases can be polygonal. The depth of the holes can have variations andthe top lateral dimension of the holes can also vary in width. Thespacing of the holes can be O (overlapping), and in some cases can rangefrom 10 nm-500 nm, and in some cases from 0 nm-300 nm, and in some casesgreater than 500 nm. The top lateral dimension of the holes can rangefrom 500 nm-2000 nm, and in some cases from 600 nm-1,600 nm, and in somecases from 600 nm-1000 nm. The holes can be periodic and/or aperiodic,and in some cases can be randomly arranged. Wavelength can range from750 nm-1000 nm, and in some cases from 800 nm-980 nm, and in some casesfrom 800 nm-900 nm. A reverse bias is applied between the P(M1) andN(M2) with bias voltages ranging from −1 volt to −100 volts or more, andin some cases from −1 volt to −35 volts. Data rate can range from 1 Gb/sto 50 Gb/s or more, and in some cases from 10 Gb/s to 25 Gb/s, and insome cases from 25 Gb/s to 50 Gb/s. In LiDAR applications the impulseresponse of the interdigitated photodiode to an impulse of light forexample to an impulse of laser light, the rise time of the impulseresponse needs to range from a few picoseconds to a few nanoseconds.Depending on the resolution of the distance needed, for example for a 30cm resolution, the rise time which is often defined as the 10-90% of thepeak response need to be 1 nsec approximately, and for higher distanceresolution, for example for a 1 cm distance resolution the rise time ofthe impulse response need to be approximately 30 psec or less. Thenumber of pulses per second for LiDAR can range from 5 pulses/second to1000 pulses/second or more. In this case the fall time can besignificantly longer than the rise time. See for example ref. Hallman etal, Detection jitter of pulsed time-of-flight lidar with dual pulsetriggering, Review of Scientific Instruments 85, 036105 (2014)

In some cases, in structures such as illustrated in FIGS. 8A-E as thereverse bias is increased the (EOE) can increase due to avalanche gainor multiplication. In some cases this lateral PIN where the I region canbe nor v can function as an avalanche photodiode and/or a single photonavalanche photodiode.

In some cases, a high-density array of these lateral PIN photodiodes canbe used for LiDAR imaging. The high-density array can have n×mphotodiodes where n and m are any digits, for example 10×10, 100×100,1,000×1,000 to name a few.

In structures such as illustrated in FIGS. 8A-E EOE can range from20%-80% or more at certain wavelengths, and in some cases EOE can rangefrom 40%-90% or more at certain wavelengths, and in some cases EOE canrange from 40% to over 100% with avalanche gain at certain wavelengths.The EOE of interdigitated photodiode with microstructure holes can begreater than the EOE of a similar interdigitated photodiode withoutmicrostructure holes at certain wavelengths.

In structures such as illustrated in FIGS. 8A-C the P well ispredominately under the M1 interdigit electrode, and the N well ispredominately under the M2 electrode, and in some cases the P and N canbe interchanged.

In structures such as illustrated in FIGS. 8A-C the width of theinterdigits M1 and M2, and in some cases more than 2 interdigits canrange from 300 nm to 3 nm, and in some cases from 150 nm to 90 nm, andin some cases from 90 nm to nm, and in some cases from 10 nm to 3 nm.

FIG. 8B shows a Ge/GeSi on Si or on SOI wafer with interdigitatedelectrodes with microstructure holes in the Ge/GeSi layer, and with alateral P, I or low dope, N structure where the P is in the Ge/GeSi andthe N is in Si. In some cases lateral PINs can also be NIPs with the Pand N interchanged. The Ge/GeSi is I or low dope and can be nor v. Thethickness of the Ge/GeSi can range from 200 nm-1000 nm or more, and insome cases 300 nm-1000 nm. The Si layer can be a n or v or I withthickness ranging from 10 nm to 1000 nm or more, and the BOX layerthickness can range from 10 nm to 2,000 nm or more on a Si substrate.The P well formed in the Ge/GeSi layer can have a well depth rangingfrom 10 nm to 1000 nm or more, and the P well is confined under the M1electrode. The N well confined under the M2 electrode in Si can have adepth ranging from 10 nm to 1000 nm or more. Microstructure holes areetched in the Ge/GeSi layer and can extend partially or entirely throughthe Ge/GeSi layer to the Si layer, and in some cases, can extend intothe Si layer. The lateral dimension of the holes can range from 600 nmto 1800 nm, and the spacing between the holes can range from 50 nm to300 nm or more. The microstructure holes can be circular, oval, square,polygonal, and/or any combination of shapes. The cross-section shape ofthe microstructure hole can be cylindrical, conical, polygonal, or anycombination of shapes. In some cases, the P well can extend beyond M1and can cover partially or entirely the top surface of the Ge/GeSi. TheSi layer under the Ge/GeSi can be N doped and in some cases N+ doped. Inthis case the PIN structure can be vertical.

In structures such as illustrated in FIGS. 8A-E, wavelength range can befrom 800 nm to 1,600 nm or more, and in some cases 800 nm-1,100 nm, andin some cases from 1,000 nm to 1A00 nm, and in some cases from 1,250 nmto 1,350 nm, and in some cases from 1,500 nm to 1,600 nm or more. Areverse bias is applied between the P and N with voltages ranging from−1V to to 100V or more, and in some cases from −1V to −35V. As thereverse bias voltage increases avalanche gain or multiplication canoccur. The EOE can range from 20% to 80%, and in some cases from 40% to90%, and in some cases from 40% to 100% or more with avalanchegain/multiplication at certain wavelengths. The EOE of microstructurehole interdigitated photodiode can have an EOE higher than a similarinterdigitated photodiode without holes at certain wavelengths. As inFIG. 8a , the microstructure holes can be periodic, aperiodic, and/orrandomly arranged. The spacing between the interdigits can be similar tothose in FIG. 8A with similar data rate bandwidth and rise time of theimpulse response. M1 can be the anode, M2 can be the cathode and areverse voltage bias is applied between M1 and M2. In some cases, thevoltage bias between M1 and M2 can be a forward bias where the voltageat M1 is larger than the voltage at M2. In some cases, avalanche gaincan be observed when M1 and M2 are reverse or forward biased howevernoise due to the avalanche gain can be lower in the case of reverse biaswhere the multiplication occurs in Si.

FIG. 8C is similar to FIG. 8B except the N well is in the Ge/GeSi layeras shown. Reverse bias is applied between P anode and N cathode. Opticalsignal can impinge from the top surface (interdigit surface) or thebottom surface, substrate surface. Wavelength of the optical signal canrange from 800 nm-1800 nm, and in some cases from 800 nm-1600 nm. Insome cases, the wavelength range is from 1000 nm-1400 nm, and in somecases from 1250 nm-1550 nm. The thickness of the Ge/GeSi can range from300 nm-1000 nm or more, and in some cases from 500 nm-1000 nm. Data ratefor optical interconnect application can range from 10 Gb/s-50 Gb/s ormore, and in some cases from Gb/s-50 Gb/s, and in some cases 100 Gb/s ormore.

In structures such as illustrated in FIGS. 8A-E, the width of theinterdigits can range from 300 nm to 100 nm, and in some cases from 100nm to 20 nm, and in some cases from 20 nm to 3 nm. In some cases thewidth of the interdigits can be greater than 300 nm.

For LiDAR applications using structures such as illustrated in FIGS.SA-E, the 10%-90% rise time can range from 1 psec to 100 psec, and insome cases from 100 pec to 1000 psec or more, and the fall time can belonger than the rise time.

With reverse bias in structures such as illustrated in FIGS. 8A-E theEQE can range from 10% to 100% or more with avalanche gain, in somecases 20%-80% with or without avalanche gain, and in some cases over100% with avalanche gain at some wavelengths. Interdigitatedphotodetectors with microstructure holes can have higher EQE than asimilar interdigitated photodetector without microstructure holes atcertain wavelengths.

FIG. 8D shows a similar structure as FIG. 8B except that the PNjunctions are replaced with metal/poly Si/semiconductor and/or metaldielectric semiconductor and/or metal semiconductor junctions. To reduceleakage current polySi and/or dielectric such as Si oxide, Al oxide, Hfoxide (layer 808) can be used between the metal and semiconductor. Theoxide or dielectric can have a thickness ranging from 0.5 nm to 5 nm ormore, and in some cases 1-2 nm. As shown in FIG. 8d a polySi layer ordielectric/oxide layer 808 can be inserted between the M1 electrode andthe Ge/GeSi to reduce leakage. In some cases, the M1 electrode can bedirectly on the Ge/GeSi. In some cases where polySi 808 is used betweenthe M1 and the Ge/GeSi interface the polySi can be doped Nor P type orundoped or lowdoped, and can have a thickness ranging from 1-100 nm ormore. As shown in FIG. 8D the M2 electrode can have a thinoxide/dielectric layer 810 between the M2 and the Si surface to form MOS(metal oxide semiconductor) junction. In some cases, the M2 can bedirectly on the Si surface to form a Schottky junction. Microstructureholes 812 are formed on the Ge/GeSi layer. The Ge/GeSi layer can have athickness ranging from 300 nm-1000 nm or more, and in some cases 300nm-900 nm. Reverse bias can be applied between the M1 and M2 electrodeswhere the M1 electrode has a more negative voltage than the M2electrode. With this bias condition avalanche gain can be observed andcan have a lower noise than biasing the M1 electrode at a higher voltagethan the M2 electrode. In some cases, a voltage can be applied to the M1and M2 electrodes where M1 electrode has a higher potential than the M2electrode, and in some cases the M1 electrode can have a lower potentialthan the M2 electrode at certain biases.

Under voltage bias condition where avalanche gain is observed it isdesirable that the avalanche gain or multiplication occurs in Si for thelowest noise in structures such as illustrated in FIG. 8B, and for thisto occur the voltage bias between M1 and M2 should be reverse biased inthe sense that M1 has a lower voltage or potential than M2.

Optical signals can impinge on the top surface (electrode surface) orfrom the bottom surface (Si substrate) in structures such as illustratedin FIGS. 8A-E. The BOX layer can be optional and in the case of Ge/GeSion Si photodetectors the BOX layer can be optional. In some cases theGe/GeSi layer can be grown in a recessed region of the Si such as atrench so that the M1 and M2 electrodes can be approximately on the sameplane.

The lateral Ge/GeSi photodetector singly or in array can bemonolithically integrated with CMOS/BiCMOS application specificintegrated circuits (ASICs) in structures such as illustrated in FIGS.8A-E. The CMOS/BiCMOS ASICs are not shown in this figure. Applicationsof Ge/GeSi on Si lateral photodetectors can include optical datacommunication, imaging and LiDAR to name a few. In the case of opticalcommunication which depends on the data rate the lateral dimension ofthe photodetector can range from 30 microns-300 microns or more, and insome cases from 20 microns to 200 microns. For imaging and/or LiDARapplications the lateral dimensions of the photodetector can range from50 microns to 1000 microns or more.

FIG. BE is similar to FIG. 8D but without microstructure holes formed.In some cases, lateral Ge/GeSi on Si photodetectors can be withmicrostructure holes and without microstructure holes on the same chipthat can be monolithically integrated with CMOS/BiCMOS ASICs. The BOXlayer can be optional for Ge/GeSi on Si photodetectors.

A mixture P and N junctions, MOS junctions, Schottky junctions, metalpolySi semiconductor junctions can be applied to lateral interdigitatedphotodetectors in any combination in structures such as illustrated inFIGS. 8A-E having both photodetectors and active electronic circuits,e.g., ASICs, on or in the same chip.

Reference Dushaq et al, Metal-germanium-metal photodetector grown onsilicon using low temperature RF-PECVD, Optics Express Vol. 25, No. 25,11 Dec. 2017 shows a metal-germanium-metal photodetector where bothelectrodes are in contact with Ge unlike in FIG. 8E, one electrode is onGe and the other electrode is on Si.

FIG. 9. is a simplified partial top view drawing of a single chip withdetector and laser arrays, and where the detectors are monolithicallyintegrated with CMOS/BiCMOS electronics, according to some embodiments.On a single Si chip 900, Si/GeSi microstructure hole photodetectors 912are monolithically integrated with CMOS/BiCMOS ASICs. The lasers 910 canbe vertical cavity surface emitting lasers or edge surface emittinglasers that can be assembled on the chip using methods such fluidicassembly. Arrays of lasers 910 at the same or different wavelength canbe used to illuminate the target in the case of LiDAR application, andthe photodetectors 912 can detect at the same wavelength or differentwavelengths. In the case of the detectors 912 detecting at differentwavelengths, band pass filters 922 can be formed on the photodetectors912 using techniques such as inkjet printing or 30 printing. In thisfigure, four example wavelengths, ?c1, ?c2, A-3, and A-4 are shown. Eachlaser 910 emits at a different wavelength ?c1, ?c2, A-3, and A-4 and thedetector array can detect at the four different wavelengths ?c1, ?c2,A-3, and A-4. Multiple lasers with the same or different wavelength canincrease the accuracy of LiDAR applications, see for example ref; Jo etal, High resolution three-dimensional flash LIDAR system using apolarization modulating Pockels cell and a micro-polarizer CCD camera,Optics Express Vol. 24, No. 26, December 2016. In order to reduceinterference from other LiDAR systems such as other automotive systems,the LiDAR signal pulses can be coded into multiple pulses, and in somecases with different wavelengths, fired at a certain sequence of singleor multiple pulses such that this coding and/or sequence can be uniqueor typically unique for individual LiDAR systems.

In structures such as illustrated in FIG. 9, for optical interconnectapplications using different wavelengths lasers and with photodetectorswith microstructure holes and with band pass filters on each of thephotodetectors that can select a different wavelength, the aggregateddata rate of this transceiver chip can range from 100 Gb/s-400 Gb/s on asingle optical fiber using coarse wavelength division multiplexing(CWDM). And in some cases wavelength division multiplexing or densewavelength division multiplexing (DWDM) can be used.

FIG. 10. is a simplified partial schematic top view drawing of a chipwith lasers and 2D array of microstructure hole photodetectors that canbe used for 3D imaging in LiDAR systems, according to some embodiments.The array of photodetectors 1012 can range from 5×5 to 1000×1000 ormore, see for example ref; Hamamatsu, Photodetectors for LiDAR,https://www.hamamatsu.com/resources/pdf/ssd/Photodetector lidarkapd0005e.pdf. The chip 1000 can contain 1 or more lasers, and in somecases no lasers are included. The photodetector array withmicrostructure holes can be monolithic integrated with CMOS/BiCMOSASICs. In some cases, band pass filters can be applied to some or all ofthe photodetector in the array for more accurate 3D imaging in LiDARapplications.

Structures as illustrated in FIG. 10, with such high density ofmicrostructure hole photodetectors can be also used in ultra-highaggregated data rate in optical interconnect applications. AggregatedData rates of 1 Tb/s can be achieved with single or multiple opticalfiber bundles or ribbons. Multiple streams of optical signal atdifferent wavelengths can be included in a single fiber using CWDM.

FIG. 11A is a partial simplified cross-section schematic of lateralphotodetector that can include both a lateral Si photodetector and alateral Ge/GeSi photodetector on a single chip that can bemonolithically integrated with CMOS/BiCMOS electronics. Thephotodetectors can be single and/or 1D or 2D arrays. The photodetectorscan be MSM and/or lateral PIN and/or lateral PIPN photodiodes that canoperate in either the photodetector mode “no multiplication or gain” orin avalanche photodiode mode with multiplication or gain, and in somecases can operate in single photon avalanche photodiode mode alsosometimes known as the Geiger mode. Ref. Renker, Geiger-mode avalanchephotodiodes, history, properties and problems, Nuclear Instruments andMethods in Physics Research A 567 (2006) 48-56. Microstructure holes canbe formed in the Si (1112) and/or Ge/GeSi (1114) photodetector. In somecases, microstructure holes may not be necessary in certainapplications, and some lateral photodetectors may not havemicrostructure holes. In some cases, the BOX layer shown in FIG. 11A canbe optional. And in some cases, one or more of the photodetectors can bea hybrid vertical structure as shown in FIGS. 2A-2D.

In some cases of structures such as illustrated in FIGS. 11A-B, M1 andM2 can be different metal such as M1 can be Al and M2 can be Cr, and insome cases M1 can be Al and M2 can be Au, Ni, Pt, W to name a few. Insome cases, M1 or M2 can be Al, Au, Ni, V, Hf, Ti, Ta to name a fewwhere M1 and M2 can have different metal or metal alloys or silicide. Insome cases, M1 and/or M2 can have an oxide layer at the interfacebetween M1 and the semiconductor such as Si and/or Ge/GeSi. In somecases, the barrier layer between M1 and/or M2 and the semiconductor canbe a material other than oxide or metal oxide or Si oxide such as Sinitride, Si carbide, to name a few. The barrier layer which can be SiOx,HfOx, TiOx to name a few or SiNx, SiC for example can have layerthickness ranging from 0.2 nm to 10 nm in some cases the barrier layercan be poly and/or amorphous Si or other semiconductor such as Ge/GeSi.The same can be applied to M3 and M4 electrodes. The Si device layer canbe low dope N or low dope P type, and in some cases intrinsic. TheGe/GeSi layer can be low dope N, or low dope P, and in some casesintrinsic. The width of M1, M2, M3, M4 can be different and can havewidth ranging from 3 nm-300 nm or more. The BOX layer in some cases canbe optional. In cases without the BOX layer the Si substrate onto whichthe Si MSM are fabricated on can be low dope N, or low dope P, orintrinsic with resistivity ranging from 1 to 100 Ohm-cm or more. In somecases the Si photodetector as in FIG. 11A can operate at wavelengthswithin a range from 700 to 1100 nm.

FIG. 11B is a simplified partial cross-section schematic of lateralphotodetectors that can include both lateral Si photodetectors and Ge/Geon Si photodetectors similar to FIG. 11A where P and N junctions areused instead of metal semiconductor Schottky junctions and/or metaloxide semiconductor junctions. The photodetectors can operate inphotodiode mode, avalanche photodiode mode, single photon avalanchemode. In some cases at least 1 photodetector can operate in thephotodiode mode, and/or at least photodetector can operate in theavalanche photodiode mode, and/or at least one photodiode can operate inthe single photon avalanche photodiode mode.

The BOX layer in FIGS. 11A-B can be optional, and the Si layer or wafercan be low dope N or low dope P or intrinsic with resistivity rangingfrom 1 to 100 Ohm-cm or more. The Ge/GeSi layer can be low dope N or lowdope P or intrinsic.

FIG. 12 is a partial cross-section of a lateral Si avalanchephotodiode/single photon avalanche photodiode with P and N junctions,according to some embodiments. The P and N junctions can extend to theBOX layer. In some cases, the lateral avalanche photodiode has a P p−PN, and in some cases Pp− N structures, and in some cases the P and Ncan be interchanged. A reverse bias is applied between the anode M1 andthe cathode M2 with bias voltage ranging from −3 volts to −200 volts,and in some cases from −10 volts to −50 volts. The p−− (n) Si layer canrange from 1 micron to 10 microns or more, and in some cases from 2microns to 10 microns. The spacing between the p+ and N+ can range from1 micron to 10 microns or more, in some cases the spacing between the p+and N+ can range from 1 to 10 microns. The lateral dimension of thephoto sensitive area which can be a diameter, or diagonal, or a side ofa rectangle, or polygon can range from 30 microns to 1000 microns ormore, and in some cases from 30 microns to 800 microns. Themicrostructure holes 1212 can be formed in the p−− Si, and in some casesthe microstructure holes can be also be formed in the doped layers suchas the P layer. The microstructure holes can be inverted pyramids,conical, cylindrical, rectangular, and/or any combination of shapes. Thespacing of the holes can range from 0 (touching, and/or overlapping) to1000 nm, and in some cases from 0 to 300 nm. The microstructure holescan have different lateral dimensions, and/or can have different depths.The microstructure holes can extend partially into the p−− (n) regionand in some cases the microstructure holes can extend to the BOX layer.The lateral dimension of the holes which can be the diameter or diagonalor one of the sides of a rectangle, can range from 500 nm to 1500 nm ormore, and in some cases from 400 nm to 1200 nm, and in some cases from600 nm to 1200 nm. Optical signals can impinge from the top surface, andin some cases from the bottom surface of the Si substrate where a windowcan be etched to the BOX layer. Optical signal can have wavelengthranging from 780 nm to 1100 nm, and in some cases 800 nm to 1000 nm.Data rate can range from 100s pluses per second to 1000s pulses persecond or more for LiDAR applications, and for Datacom applications from1 Gb/s to 25 Gb/s or more. In some cases, for operations using plasticoptical fiber the data rate can range from 100 Mb/s to 10s Gb/s. In somecases, the APO/SPAD can operate as a photodiode without gain and in somecases can operate as an avalanche photodiode with multiplication factorgreater than 1, and in some cases with multiplication factor greaterthan 10, and in some cases with multiplication factor ranging from 1 to1000 or more. In the SPAD mode the multiplication factor can range from500 to 100,000 or more. In some cases, the Si APO/SPAD can be a 1Dand/or 2D array that can be monolithically integrated with CMOS/BiCMOSASICs. The 2D array of PD/APO/SPAD can be used for imaging and/or 3Dimaging. For conventional Si APO see for example ref. Laforce, Low noiseoptical receiver using Si APO, SPIE vol. 7212, 721210 (Feb. 6, 2009)ref. Hamamatsu technical information SD-28 Characteristics and use of SiAPO (avalanche photodiode), where the I or low dope layer can range inthickness from 20-100 microns.

In some applications microstructure holes may not be necessary as inFIGS. 3A, 4A, 5A, and in some cases photodetectors with microstructureholes and photodetectors without microstructure holes can exist on thesame chip that is monolithically integrated with CMOS/BiCMOS ASICs. Thiscan apply for devices shown in FIGS. 11A, 11B and 12. In some cases themicrostructure hole photodetector and/or photodetectors withoutmicrostructure holes can be monolithically integrated with CMOS/BiCMOSASICs.

In structures such as illustrated in FIG. 12, a reverse bias can beapplied between the anode M1 and cathode M2 with voltages ranging from−3 to −100 or more, and in some cases −3 to −45 volts. In some cases, M1and/or M2 can form Schottky contacts, and in some cases M1 or M2 canform metal oxide semiconductor junctions, and in some cases M1 and/or M2can form P and/or N junctions. In some cases where the junctions areeither Schottky and/or MOS (metal oxide semiconductor) the currentvoltage characteristics can be symmetric and/or almost symmetric suchthat gain such as avalanche gain can be observed in the forward and/orreverse voltage bias directions for APO/SPAD.

Lateral photodetector with microstructure holes can have a higher EOEthan a comparable lateral photodetector without microstructure holes atcertain wavelengths, and/or at certain bias voltages.

In the case where PN junctions are formed and where one of theinterdigit electrodes is formed on a P junction for example such as M1and shown in FIG. 12, and a second set of interdigit electrodes formedon N junction the lateral photodiode are operated with a reverse biasvoltage between the anode (M1) and cathode (M2) for PD/APO/SPAD.

The microstructure holes in some cases can be in the I or low dope P Siregion, and in some cases can also be in the P region in structures suchas illustrated in FIG. 12. The microstructure holes can extend partiallyinto the I or low dope P region, and in some cases can extend to the BOXlayer. In some cases microstructure holes in the P or low dope regionmay not be necessary and super structures can be fabricated on thesurface of the P or low dope region that can be made of high indexdielectrics such as Hf oxide. In FIG. 12 the P+, P, N+ can extendpartially into the device layer, and in some cases can extend to the BOXlayer. Ref liyama et al, Silicon Lateral Photodiodes Fabricated byStandard 0.18 microns CMOS Process, ECOC 2009, September 2009, Vienna,Austria, shows a lateral avalanche photodiode without microstructureholes to enhance absorption. Reference Wegrzecka et al, Design andproperties of Silicon avalanche photodiodes Opto-electronics Review 12(1), 95-104 (2004).

FIGS. 13A-B show laser pulses that can have a certain sequence of pulsesfor LiDAR applications in order to distinguish between different LiDARsignals that may exist in the same environment. In some cases, thesequence of optical pulses, such as shown in FIG. 13A can be coded tofurther distinguish from signals of other LiDAR units operating in thevicinity. The set of pulses depicted in FIG. 13B are the reflectedoptical signals as detected by the LiDAR photodetectors. This receivedsequence of electrical signals can be compared to the sequence ofoutgoing optical signals to authenticate that these optical pulses andelectrical signals are from the same LiDAR unit. The coding schemes canbe as illustrated, with pulse position modulation, or pulse widthmodulation, or wavelength modulation, to name a few.

The wavelength of the optical signal which can originate from a laser orlight emitting diode (LED) can range from 800 nm to 1800 nm, and in somecases the optical pulses can have all the same wavelength, and in somecases the optical pulses can have different wavelength. In the casewhere plural optical pulses have different wavelength the respectivephotodetectors on the same chip can have bandpass filters to detect theselected wavelengths of the reflected optical pulses.

In some cases, more than one light source such as lasers or LEDs can beused to improve accuracy of imaging in LiDAR applications, see forexample, ref. Chen et al, Accuracy improvement of imaging lidar based ontime-correlated single-photon counting using three laser beams, OpticsCommunications, https://doi.org/10.1016/j.optcom.2018.08.017

FIGS. 14A-C include two plots in FIG. 14B and FIG. 14C that showexperimental results for vertical PIN microstructure hole photodetectorshown in FIG. 14A. The PIN Si microstructure hole photodetector shown inFIG. 14A has an I or low dope layer of thickness 1-2 microns a N+ Silayer with a thickness of approximately 0.5 microns and a top p+ Silayer of approximately 0.3 microns with microstructure holes 1412 thatare inverted pyramids with lateral dimension of approximately 600-800 nmwith spacing of approximately 100 nm. The anode is formed on the P layerand the cathode is formed on the N layer, and a reverse bias is appliedbetween the anode and cathode.

FIG. 14B shows responsivity as a function of reverse bias for opticalsignal at 850 nm. Curve 1422 is for the photodiode withoutmicrostructure holes and curve 1420 is for the photodiode withmicrostructure holes. As can be seen the photodiode with microstructureholes has a higher responsivity by almost a factor of three over asimilar photodetector without microstructure holes. In addition, thegain or increase in responsivity for microstructure hole photodiodeoperating in the avalanche photodiode mode achieve gain ormultiplication at a lower voltage than a similar photodiode withoutmicrostructure holes.

FIG. 14C shows similar curves as FIG. 14B except instead of responsivitymultiplication is shown. Curve 1432 is for the photodiode withoutmicrostructure holes and curve 1430 is for the photodiode withmicrostructure holes. Multiplication for microstructure hole avalanchephotodiode is over 1000 compared to a similar photodiode withoutmicrostructure holes the multiplication is less than 700.

The microstructure holes can enhance the electric field such thatavalanche effects can occur at the lower voltage and with the higherfield avalanche gain and/or multiplication can be higher than a similarphotodiode without microstructure holes at the same voltage for example.In some cases, lateral structures PIN and/or PIPN microstructure holephotodiodes operating in the avalanche mode can have higher avalanchegain and/or multiplication than a similar photodiode withoutmicrostructure holes at a given reverse bias voltage. In some cases MSMlateral photodetectors can also exhibit avalanche gain at forward orreverse bias, and can have a higher avalanche gain and/or multiplicationthan a similar photodetector without microstructure holes at a givenvoltage.

With the addition of microstructure holes in vertical or lateralphotodetectors described in this patent specification, the absorptionlayer which often is the I or low dope layer, and in some cases dopedlayers, can be thin with thickness ranging from 300 nm-5,000 nm, and insome cases from 500 nm-2,000 nm and can achieve a higher externalquantum efficiency than a comparable photodetector withoutmicrostructure holes at certain wavelengths. In the case of APO/SPAD ofeither the vertical or lateral microstructure hole photodetectorstructures, the absorption region or layer can be 10× thinner than aconventional Si APO/SPAD at certain wavelengths. In some cases, it canbe greater than 10× thinner, and in some cases it can be greater than 5×thinner to achieve comparable responsivity and/or multiplication atcertain wavelengths. In addition, the microstructure hole APO/SPAD canhave lower reverse bias voltage to achieve responsivity and/ormultiplication as compared to a conventional Si APO/SPAD.

Silicon avalanche photodiode monolithically integrated with CMOS/BiCMOSASICs with high multiplication are discusses for example in reference;Youn et al, A 12.5 Gb/s SiGe BiCMOS Optical Receiver with aMonolithically Integrated 850-nm Avalanche Photodetector, OFC/NFOECTechnical Digest 2012 OSA; where their responsivity is of the order of0.01 A/W or less for multiplication factor of 1 at 850 nm.

FIGS. 15A-B are plots showing experimental current-voltage (IV)characteristics of lateral interdigit Si MSM or Schottky contacts withand without native oxide, according to some embodiments. The Si layer islow P type doping with resistivity range of 10-20 Ohm-cm.

In FIG. 15A, curve 1510 shows a S type characteristic with illuminationat 850 nm wavelength, where native oxide was removed with a buffer oxideetch and Al interdigits deposited. In FIG. 15B, curve 1520 shows a diodelike characteristic when illuminated at 850 nm wavelength where nativeSi oxide was not removed and Al interdigits were deposited. Dark(non-illuminated) curves 1512 and 1522 are shown in FIGS. 15A and 15B,respectively.

The diode like IV characteristics as in FIG. 15B can have higher EOE andcan have avalanche gain such that the EOE can be 100% or more at lowbias of +/−3 volts or more. The spacing between the Al interdigits wasapproximately 1 micrometer, and the width of the interdigits isapproximately 300 nanometers.

The structure of FIG. 15A can have gain such as photoconductive gain,and in some cases at higher bias can have avalanche gain. The structureof FIG. 15B can have avalanche gain at higher bias. Reference Li, et al.Silicon photodiodes with high photoconductive gain at room temperature,Optics Express, Vol. 20, No. 5 27 Feb. 2012.

FIGS. 16A-16D are experimental gain plots of an Si microstructure holePIN photodiode in a vertical configuration. The plots show experimentalavalanche gain at different wavelength from 850 nm to 990 nmillumination of microstructure hole photodiode as compared to a similarphotodiode without microstructure holes.

FIG. 16A shows experimental gain for illumination at 850 nm@ ˜8 μW.Curve 1610 shows the microstructure hole PIN photodiode responsivity ofapproximately 80 A/W at approximately 30 volts reverse bias as comparedto a similar Si PIN photodiode without holes with responsivity ofapproximately 0.3 A/W at approximately 30 volts reverse bias (curve1612). The microstructure holes in FIG. 16A-16D have a diameter of 700nm and a period of 1000 nm in a square lattice.

FIG. 16B shows experimental gain for the same device under 900 nmwavelength illumination @ ˜8 ρW. FIG. 16C shows the same device with 940nm wavelength surface illumination 940 nm @ ˜15 μW. FIG. 160 shows thesame device with 990 nm wavelength surface illumination nm @ ˜10 ρW. Inall cases the onset of avalanche gain with microstructure holephotodiode occur at a lower reverse bias voltage than a similar Siphotodiode without holes. The responsivity of microstructure holephotodiode can be higher than the responsivity of a similar photodiodewithout microstructure holes at certain bias voltages.

FIGS. 17A-17H are plots of shows FDTD (finite difference time domain)simulation of the optical field of various microstructure holestructures that can be either in a vertical or a lateral configuration,according to some embodiments. FIG. 17A shows an FDTD simulation of theoptical field of a microstructure hole structure that has 400 nm Ge onSi bulk wafer of 675 micron thickness. The microstructure holes are in asquare lattice with a period of 400 nm and a diameter of 1100 nm.Cylindrical holes are etched to a depth of 200 nm. The vertical axisshows absorption in the Ge layer and the horizontal axis shows thewavelength. The absorption is directly proportional to the externalquantum efficiency (EQE). The ratio of EQE/absorption can range from0.1-1. In cases where photo generated carriers are not lost torecombination and can be collected efficiently, the EQE can beapproximately equal to the absorption, or equivalently the ratioEOE/absorption can range from 0.8-1. The optical signal is surfaceilluminated (microstructure hole side of the wafer) at normal incidence.The absorption or EQE can be 60% or higher at certain wavelength rangeof 700 nm-1350 nm, and in some cases the absorption or EQE can be 40% orgreater at certain wavelength range of 700 nm to 1350 nm. Microstructurehole PD/APO/SPAD can have a higher EQE than a comparable PD/APO/SPADwithout microstructure holes at certain wavelengths and/or at certainbias voltages.

FIG. 17B shows a FDTD simulation of the optical field in microstructurehole Ge on Si. The optical signal illuminates the hole surface averagedover an angular distribution of +10 to −10 degree or normal incidence.The Ge layer is 800 nm thick on Si wafer. Cylindrical holes are formedto a depth of 400 nm. The solid curve 1720 is for holes with 1000 nmdiameter and 1400 nm period in a square lattice, and the dashed curve1722 are for holes with 1200 nm diameter and 1600 nm period in a squarelattice. The vertical axis in absorption in the Ge layer, and thehorizontal axis is wavelength from 800 to 1800 nm. Absorption and/or EQEcan be greater than 40% at some wavelengths in the range of 800-1800 nm.

FIG. 17C shows a FDTD simulation of optical field of microstructureholes in Ge on Si. The Ge layer is 600 nm on Si wafer. Cylindrical holeswith diameter 1200 nm and period 1600 nm in a square lattice with holedepth of 300 nm is shown in the solid curve 1730. The dashed curve 1732shows holes with 1000 nm diameter and 1400 nm period in a squarelattice. The absorption and/or EQE can be 30% or higher at certainwavelength in the range of 800-1800 nm.

FIG. 17D is similar to FIG. 17c with an added Ge strain of approximately0.2%.

FIG. 17E is similar to FIG. 17B with the cylindrical holes etched to theSi wafer or a depth of 800 nm.

FIG. 17F is similar to FIG. 17C except with cylindrical holes etched tothe Si or a depth of 600 nm.

FIG. 17G is similar to FIG. 17C except with the cylindrical holes etchedthrough the Ge into the Si to a total depth of 800 nm.

FIG. 17H is similar to FIG. 17B except with the cylindrical holes etchedthough the Ge into the Si with a total depth of 1000 nm.

In all FIGS. 17A-17H the incident optical field is averaged over −10 to10 degrees normal to the surface. The absorption and/or EQE can be 40%or higher at certain wavelength in the wavelength range of 800-1800 nm

FIGS. 18A-B are simplified partial cross-sections of a lateralinterdigitated photodetector with metal oxide semiconductor (MOS)junctions, according to some embodiments. In FIG. 18A, the M1 and M2 areAl electrodes and a 2 nm Al oxide layer 1808. Al Oxide 1809 is formed onSi using atomic layer deposition. The Si substrate or layer is low dopeP type with a resistivity of 10-30 Ohm/cm, and in some cases greaterthan or equal to 10 Ohm/cm. The Al electrodes are deposited on the Aloxide 1808 with a width of 300 nm, and in some cases the width can rangefrom 5 nm-600 nm. The spacing between the electrodes M1 and M2 can rangefrom 100 nm to 10,000 nm or more, and in some cases the spacing canrange from 30 nm-1,000 nm. In some cases, the spacing can be less than30 nm. Light can be incident on the top surface containing theelectrodes, and in some cases, light can be incident from the substrateside or the bottom surface. Bias can be applied to the M1 and M2electrodes in either the forward or reverse direction. Wavelength rangefor the interdigit photodetector can range from 600 nm-1100 nm, and insome cases less than 600 nm.

FIG. 18B is similar to FIG. 18A with the addition of a BOX layer,thickness can range from 10 nm-2000 nm or more. The Si device layer ontop of the BOX can be intrinsic or low dope P or N type with resistivityof 1 Ohm/cm or greater with a thickness range of 100 nm-5000 nm or more.An oxide layer such as Si oxide, Al oxide, Hf oxide, Ti oxide, Ta oxide,to name a few can be formed on the Si device layer. The oxide layer canhave a thickness ranging from 1 nm-5 nm, and in some cases greater than5 nm. In some cases, the oxide can be a dielectric layer other thanoxide such as carbide, for example Si carbide, W carbide, and in somecases can be a nitride layer, for example Si nitride. Metal electrodesare formed on the oxide layer to form a MOS junction. In some cases, oneof the electrodes can be MOS junction, and the other electrode can be aSchottky junction. Microstructure holes 1812 can be formed on thesurface with etch depth into the Si device layer, and in some casesthrough the Si device layer to the BOX layer. The microstructure holescan be cylindrical, funnel, inverted pyramids, conical, rectangular,amoebic, and polygonal, or any combination thereof. The lateraldimension of the microstructure hole at the surface can range from 500nm-1200 nm. The spacing between the holes can range from 0 nm-1000 nm ormore, and in some cases 0 nm-500 nm. The holes can be fully or partiallyfilled with dielectric such as Si oxide, Si nitride, Al oxide to name afew. A voltage bias can be applied between M1 and M2 electrodes ineither the forward or reverse bias. The polarity of the voltage bias ischose to optimize the performance of the interdigitated lateralphotodetector performance, for example high EQE, high speed, high gain,low noise to name a few. M1 and M2 can be metal forming MOS junctions,the metal can include, Al, Cu, W, Mo, Ni, Cr, Pt, Au, to name a few, andin some cases, can be metal alloys, and in some cases can be metalsilicide. Light can impinge on the top surface (electrode surface) or insome cases from the bottom surface (substrate surface). In some casesthe BOX layer can be optional.

FIG. 19 is a simplified partial cross-section of an interdigitatedlateral photodetector, according to some embodiments. The lateralphotodetector can be a photodiode, an avalanche photodiode, or a singlephoton avalanche photodiode with proper P and N doping profiles such asPN, PIN, PIPN to name a few. A reverse bias is applied between the anode(M1) and cathode (M2). The interdigitated electrode can be metal and/ormetal silicides. The interdigitated photodetector is fabricated on a Sion insulator wafer (SOI) and where the photodetector with itsinterdigitated electrodes is buried with amorphous Si, and wheremicrostructure holes are formed in the amorphous Si and where theamorphous Si (a-Si) and the microstructure holes 1912 can be buried withan oxide or dielectric such as Si dioxide. The lateral dimension of themicrostructure holes 1912 can be larger than the spacing between theinterdigitated electrodes, and in some cases can include multipleelectrodes within the lateral dimensions of the microstructure hole.Light impinges on the top surface opposite from the substrate surface.Arrays of photodetectors can be fabricated and connected to CMOS ASICson a single chip. The thickness of the BOX layer can range from 10 nm to2000 nm or more, and the thickness of the crystalline device layer whichcan be I or low dope P or N can have a thickness ranging from 10 nm to100 nm and in some cases from 30 nm to 300 nm, and in some cases from 50nm to 500 nm, and in some cases from 500 nm to 1000 nm. The depth of theP and N wells can be formed partially into the device layer or entirelyin the device layer to the BOX layer. The spacing between the electrodesM1 and M2 can range from 100 nm to 1000 nm, and in some cases more than1000 nm. In some cases, the spacing between the M1 and M2 electrodes canbe periodic, and in some cases aperiodic, and in some cases random. Pand N wells can be formed under the electrode, and in some cases the Pand N doping can extend beyond the width of the electrode and in somecases the doping can include PIPN for example. The thickness of theelectrodes can range from 50 nm to 500 nm, and in some cases to 1000 nmor more. The a-Si can be deposited on the photodetector using plasmaenhanced chemical vapor deposition, chemical vapor deposition, thermaldeposition such as electron beam and/or any other methods used in CMOSprocessing. The thickness of the a-Si can range from 100 nm-1000 nm andin some cases more than 1000 nm. The microstructure holes can becircular, rectangular, oval, and/or any other shapes, and can becylindrical, trapezoidal, conical, and/or any combination ofcross-section, and can have a surface lateral dimension ranging from 400nm to 1300 nm and in some cases 700 nm-1000 nm. The microstructure holes1912 and the a-Si can be partially or entirely buried by dielectric witha refractive index different from the a-Si for example Si dioxide, Sinitride to name a few. The reverse bias can have a voltage range of 1V-35 V, and in some cases 0.7 V-3.3 V, and in some cases 3.3 V-15 V. Thewavelength range of the incident photon that can be modulated signalsuch as for data communication or reflected signal such as fortime-of-flight applications or optical images can range from 700 nm to1100 nm.

The lateral dimension of microstructure holes 1912 in most casesmentioned in this patent specification are for microstructure holes notfilled with any dielectric, e.g., filled only with air or vacuum wherethe optical refractive index is approximately 1. In the cases where themicrostructure holes are filled fully or partially with the dielectricthe lateral dimension of the microstructure hole can be reduced by theeffective optical refractive index of the dielectric/voids in themicrostructure holes. For example, a microstructure hole with lateraldimension of 800 nm that is not filled (e.g., in air) can have a lateraldimension of 533 nm when completely filled with SiO2 which has anoptical refractive index of approximately 1.5. Microstructure holelateral dimensions can in some cases be reduced when filled withdialectic, where the refractive index is greater than 1 for example(lateral dimension of microstructure hole in vacuum or air)/(opticalrefractive index), and in some cases where the microstructure hole ispartially filled with dielectric an effective optical refractive indexcan be calculated by the ratio of the volume of 1 or more dielectrics inthe microstructure hole.

FIGS. 20A-D are schematics of a LiDAR and/or camera system whereindetector arrays are monolithically integrated with CMOS/BiCMOS ASICs onone or more chips, according to some embodiments. In FIG. 20A, detectorarray 2050 can be monolithically integrated with CMOS/BiCMOS ASICs 2060and where the detector array 2050 can be a charged coupled device (CCD),CMOS based imager, photodetector, APO and/or SPAD. The laser sources2040 can be assembled on the Si chip 2030 using fluidic and/or roboticassembly, and the electrical connections to the laser can be a back endof line (BEOL) process. The light source can be light emitting diodes(LED) laser diodes which can be edge surface emitting lasers, verticalcavity service emitting lasers, and/or any combination thereof. Thelight source single or multiple beam can be directed to scanning MEMSmirror 2020 such that a raster scan can be performed to illuminate atarget object (outgoing light beam 2042 to target 2010), and the lightsource reflected from the target object (incoming light beam from target2052) can be imaged onto detector arrays 2050. The Si micro mirrors 2020for use in the raster scan can be a separate chip mounted above thelight source. For example, see reference, Hofmann, MEMS mirror for lowcost laser scanners, Fraunhofer, www.minifaros.eu

In some cases, the light source in the examples illustrated in FIGS.20A-D can be pulsed or CW (constant wave) to illuminate target objectsat certain wavelengths, with wavelengths ranging from 800-1600 nm. Thereflected light from the target object that is illuminated by the lightsource can be focused into a detector array and can be a camera elementusing CCD and/or CMOS sensors. And in some cases, for higher sensitivitythe sensor array can be APO/SPAD arrays.

In some cases, the light source in the examples illustrated in FIGS.20A-D can be pulsed and a time of flight of the light pulse to thetarget object and detected by the detector array can be used in a LiDARmode. With multiple laser beams and with MEMS micro mirror scanners 2020a raster scan can be performed with greater spatial resolution, andshorter time than a single beam LiDAR. Only the very basic elements areshown, not shown are lens, micro mirror drivers, and other elementsnecessary to complete an imaging and/or LiDAR system. Single and/ormultiple wavelengths of the light source can be used and the detectorarray can have filters to detect single or multiple wavelengths. In somecases, multiple arrays can be fabricated on a single Si chip withappropriate filters over each array to detect certain wavelengths. Ref.Vasile et al, Photon Detection with High Gain Avalanche PhotodiodeArrays, IEEE transactions on Nuclear Science, Vol. 45, No. 3, June 1998.According to some embodiments the Ge photodetectors can have wavelengthranges from 700-2200 nm and the Si photodetectors can have wavelengthranges from 700-1100 nm. According to some embodiments, the Siphotodetectors can operate at one or more of the following wavelengths:905 nm, 940 nm, 980 nm and 1040 nm. According to some embodiments, theGe/GeSi photodetectors can operate at one or more of the followingwavelengths: 905 nm, 940 nm, 980 nm, 1040 nm, 1550 nm, 1650 nm and 1850nm.

FIG. 20B is similar to FIG. 20A with the exception that the light sourcearray is on one chip 2032 and the detector array or arrays on a separatechip 2034. Note that in this case each of the chips 2032 and 2034 havetheir own respective CMOS/BiCMOS ASICs 2060 and 2062. In some cases,multiple light source arrays, and multiple detector arrays can be usedat 1 or more wavelength to improve 3D sensing of target objects and tominimize interference from other sources such as the sun.

FIG. 20C shows a simplified schematic of a LiDAR system similar to FIG.20B where array of light emitters such as surface emitting lasers withscanning micro-mirrors such as MEMS mirrors scans a target such as a carwith multiple beams at the same or different wavelength and thereflected beam can impinge on 2 sets of high density 2D array ofPD/APO/SPAD that are monolithically integrated with CMOS/BiCMOS ASICs.The high-density detector arrays 2034 and 2036 can be spaced apart by 2to 20 cm or more to provide additional depth information, and in somecases more than 2 high density photodetector arrays can be used toprovide additional depth information. In some cases the illuminator canbe LED and/or lasers and can be used in addition to LiDAR mode and/oruse to illuminate a target and the high density detector arrays canfunction in a manner similar to a camera and with the use of 2 or morehigh density arrays set apart by 6 or more cm can provide depthinformation such as 3D imaging similar to human eyes.

FIG. 20D shows a simplified schematic or a LiDAR and/or camera systemwhere a high density array of illuminators such as surface emittinglasers 2042 can be used to illuminate the target 2010 and the reflectionfrom the target impinges on a high density detector array 2038. In somecases the high density light emitters and the high density photodetectorarray can be implemented on a single Si chip where the detectors aremonolithically integrated with CMOS/BiCMOS ASICs 2066, and where theemitter can be fabricated on the Si chip using selective hetero epitaxyof 111-V material, wafer bonding of 111-V material to Si, fluidic selfassembly. In some case more than one CMOS/BiCMOS ASICs can be integratedas shown with CMOS/BiCMOS ASICs 2064. In some cases, the high densityemitter and the high density detector array can be separate chips, andin some cases as in FIG. 20C multiple arrays of detectors spaced apartcan be used to provide depth information. In some cases multiple highdensity arrays of optical emitters can be used. In some cases micromirrors for scanning can be omitted.

SPAD monolithically integrated with CMOS ASICs are discussed inreference Zhang et al, A CMOS SPAD Imager with Collision Detection and128 Dynamically Reallocating TDCs for Single-Photon Counting and 3DTime-of-Flight Imaging, Sensors 2018, 18, 4016; doi: 10.3390/s18114016.

Flash LiDAR can be implemented in some cases without the use of scanningmirrors; see for example reference, Baba et al, Development of an InGaAsSPAD 2D array for flash LIDAR, doi: 10.1117/12.2289270

Reference Beer et al, SPAD-based flash LiDAR sensor with high ambientlight rejection for automotive applications, Proc. Of SPIE Vol. 105401054028-3; discusses using SPAD photodetectors for flash LiDARapplications.

Reference Niclass et al, Design and characterization of a 256×64-pixelsingle-photon imager in CMOS for a MEMS-based laser scanningtime-of-flight sensor, Optics Express, 11863 Vol. 20, No. 11, 21 May2012; discusses using SPAD array for imaging integrated with CMOS ASICsthat can be used either as a flash LiDAR or a scanning LiDAR. In Niclassreference FIG. 3 a cross-section of the SPAD is shown, however theaddition of microstructure holes in the deep N well and/or into the Psubstrate can enhance the absorption of the near infrared photons asdescribed in this patent specification.

Monolithic integration of a thick Si photodetector with CMOS ASICs canbe implemented by using the substrate as a photodetector, see forexample reference; Lee et. al, A Back-Illuminated Tim-of-Flight ImageSensor with SOI-Based Fully Depleted Detector Technology for LiDARApplication, Proceedings 2018, 2, 789; doi:10.3390/proceedings2130789;however due to the thickness of the Si absorption layer the 10-90% risetime of the photodetector is in the nanosecond range. This can restrictthe depth resolution to approximately 1 meter or more.

FIGS. 21A-21C are simplified partial schematic cross-sections of alateral APO/SPAD Ge/GeSi on Si where the absorption of the opticalsignal are predominately in the Ge/GeSi and the multiplication such asavalanche gain occurs in the Si, according to some embodiments. Thelateral APO/SPAD is surface illuminated where light can impinge on thetop surface, and in some cases can impinge from the bottom surface(substrate surface), and in some cases the substrate can be thin and/ora via can be etched for a bottom illumination. In FIG. 21A, thestructure consists of Ge/GeSi that can be selective area grown on I orlow dope P Si (re). And in some cases, the Ge/GeSi can be grownuniformly on the I or low dope Si layer and Ge/GeSi can be etched inareas where the M2 or cathode 2122 is formed. P and N+ regions can beformed in the I or low dope Si, and interdigit M2 2122 can form an ohmiccontact with the W region. The Ge/GeSi on the I or low dope Si can havea thickness ranging from 200 to 2,000 nm or more, and in some cases300-1,000 nm, and can be I or low dope P or N type and p+ Ge/GeSi layeror region 2130 can be formed on the I or low dope Ge. The P Ge/GeSi 2130can have a thickness ranging from 10 nm to 300 nm or more and M1interdigit electrodes 2120 can be formed on the P Ge 2130 forming anohmic contact. In some cases, multiple M1 2120 can be formed on the PGe/GeSi 2130. Microstructure holes 2112 can be etched into the P Ge 2130and in some cases through the P Ge 2130 into the I or low dope Ge, andin some cases through the I or low dope Ge to the I or low dope Si. Thecross-section of holes 2112 can be cylindrical, rectangular,trapezoidal, conical, to name a few, and can have a lateral dimension atthe surface ranging from 600 nm to 1500 nm or more, and in some cases800 nm-1400 nm. The spacing between the adjacent holes 2112 can rangefrom 0 nm (touching and/or overlapping) to 1000 nm or more, and in somecases 100 nm-600 nm. The holes can be periodic, and/or aperiodic, and/orrandomly spaced. A reverse bias is applied between M1 (anode) 2120 andM2 (cathode) 2122. Electric field extends from p+ Ge/GeSi 2130 thoughthe I or low dope Ge/GeSi and through the I or low dope Si to the N+.

Ref. Novak et al, Lateral Avalanche Photodetector USPTO 2017/0338367 A1,discusses a lateral structure where the Ge is not electrically connectedto an anode or cathode and operate predominately in a waveguide mode. Inthe current patent specification the Ge/GeSi is connected directly to ananode and/or cathode, as illustrated for example in FIGS. 21A-C andwhere electric fields penetrate from the p+ region to the N+ region, andwhere in addition optical signal is surface illuminated.

The wavelength range in devices as illustrated in FIGS. 21A-C can rangefrom 800 nm to 1700 nm, and in some cases 800 nm-1800 nm, and in somecases 1100 nm-1550 nm, and in some cases 1150 nm-1550 nm. A reverse biasvoltage is applied between the anode and cathode with a reverse biasvoltage ranging from −2 volts to −50 volts or more, and in some casesfrom −10 volts to −45 volts. The BOX layer can be optional.

Ref Zhu et al, Waveguided Ge/Si Avalanche Photodiode With SeparateVertical SEG-Ge Absorption, Lateral Si Charge, and MultiplicationConfiguration, IEEE Electron Device Letter, Vol. 30, No. 9, September2009, discusses a lateral Ge on Si APO where the light is coupled in awaveguide mode.

FIG. 21B is similar to FIG. 21A with the exception that the Si layer isN or N+ and M2 forms and ohmic contact to the N or N+ Si.

FIG. 21C is similar to FIG. 21B with the P and N interchanged (so thatelectrodes M2 are anodes 2016, and electrodes M1 are cathodes 2124).

FIGS. 21B and 21C can operate in the reverse bias, where reverse biasvoltage is applied between the anode and cathode, with bias voltageranging from −1 to −10 volts or more, and in some cases avalanche gaincan occur at higher reverse bias voltages.

The lateral PD/APO/SPAD Ge/GeSi on Si photodetectors illustrated inFIGS. 21A-C can be monolithically integrated with CMOS/BiCMOS ASICs forsignal processing and/or enhancement, and/or transmission.

Microstructure hole lateral PD/ADP/SPAD such as illustrated in FIGS.21A-C can have a higher EOE than a comparable lateral PD/APO/SPADwithout microstructure holes at certain wavelengths and/or at certainbias voltages. In some cases, microstructure holes may not be necessaryfor certain applications.

Lateral interdigitated PD/ADP/SPAD xxsy [such as shown in which FIGS.21A-C can be fabricated in arrays or multiple arrays, and in some caseshigh density arrays of 1000×1000 photodetectors or more, andmonolithically integrated with CMOS/BiCMOS ASICs electronics forapplications in optical interconnect, imaging, 30 imaging, and/or LiDAR.

FIG. 22A shows a simplified cross-section schematic of a interdigitatedvertical Ge/GeSi on Si APO/SPAD with or without BOX layer, according tosome embodiments. On a N+ Si device layer or a N+ Si substrate a P layerSi can be epitaxial grown followed by an I or low dope Si, followed by Ior low dope Ge layer with or without a low temperature Ge/GeSi bufferlayer, followed by a p+ Ge/GeSi layer 2210. Thicknesses of the P Silayer can range from 5 to 100 nm, the I or low dope Si thickness canrange from 5 to 500 nm, and the I or low dope Ge thickness can rangefrom 50 to 1000 nm or more. The p+ Ge 2210 thickness can range from 10to 300 nm. Interdigitated anodes 2220 are formed on the p+ Ge 2210 andinterdigitated cathodes 2222 are formed on the N+ Si. A reverse biasvoltage is applied between the anode and cathode. The width of the anodeand cathode interdigits can range from 5 nm to 300 nm or more. Thethickness of the interdigit anode, cathode electrodes can range from 50to 300 nm or more, and can be metal, or metal alloy, or a silicide.Microstructure holes 2212 can be etched into the p+ Ge layer through thep+ Ge layer 2210 and into the I or low dope Ge/GeSi layer and/or themicrostructure hole can be etched to the I or low dope Si layer. In somecases, the microstructure holes 2212 can be etched into the Si. Lightcan impinge on the top surface and/or from the bottom surface (substrateside). The wavelength can range from 750 nm to 1800 nm and in some cases850 nm-1550 nm, and in some cases 1040 nm-1550 nm. Data rates can rangefrom 1 Gb/s or less to 50 Gb/s or more.

The microstructure holes 2212 can be cylindrical, trapezoidal,rectangular, inverted pyramids, funnel, and can have diameter rangingfrom 600 nm-1700 nm or more, and in some cases 600 nm-1300 nm. Thespacing between the holes can range from 100 nm-500 nm, and in somecases more than 500 nm. The microstructure holes can be arranged in aperiodic lattice such as a square or hexagonal lattice, and in somecases the microstructure holes can be aperiodic and/or random in bothspacing and/or shape and/or depth.

FIG. 22B shows a simplified top view of the structure shown in FIG. 22Awhere the interdigit anodes and cathodes are connected to a transmissionline and can be monolithically integrated with CMOS/BiCMOS ASICs,according to some embodiments.

FIGS. 23A-B, 24A-B, 25A-B and 26A-B are schematic cross-sections ofinterdigitated lateral Ge/GeSi on Si APDs/SPADs, according to someembodiments. In FIG. 23A shows an interdigitated lateral Ge/GeSi onSiPIPN APO/SPAD. The lateral Ge/GeSi APO/SPAD can be formed on a I orlow dope Si substrate or on a I or low dope Si device layer on a SOIwafer. The I or low dope Si can be low dope N or low dope P as shown inFIG. 23A the Si layer is low dope P or 1c. P and N+ wells can be formedin the Si layer with the M2 electrode forming an ohmic contact with theN+ well. The I or low dope Ge/GeSi 2310 can be selective area grown onthe I or low dope Si with thickness ranging from 100 nm-1000 nm or more.p+ well can be formed in the Ge/GeSi 2310 and the M1 interdigitelectrode can form an ohmic contact with the p+ Ge/GeSi well. The widthof the Ge strip 2310 can range from 200 nm to 2000 nm or more, and insome cases the width of the Ge/GeSi strip can range from 1000 nm to10,000 nm or more. The length of the Ge/GeSi strip can range from 1micron to 1000 microns or more, and in some cases from 20 microns to1000 microns or more, and in some cases to 10,000 microns or more. Thewidth of the interdigit electrodes M1 and M2 can range from 5 nm to 300nm or more. The depth of the p+ well in the Ge/GeSi can be partiallyinto the Ge/GeSi, and in some cases through the entire depth of theGe/GeSi 2310. The P and N+ well in Si can be partially in the I or lowdope Si device layer, and in some cases extending to the bottom of the Ior low dope Si device layer to the BOX layer. A reverse bias voltage isapplied between M1 (anode) and M2 (cathode). M1 and M2 are connected toa transmission line that carries the electrical signal to CMOS/BiCMOSASICs integrated with the APO/SPAD detectors or detector array. Lightcan impinge from the top surface, and in some cases from the bottomsurface. The wavelength of light can range from 800 nm-1800 nm, and insome cases from 1040 nm to 1550 nm, and in some cases from 900 nm to1350 nm. Data rate can range from less than 1 Gb/s to greater than 50Gb/s, and in some cases from 10 Gb/s to 50 Gb/s, and in some cases to100 Gb/s or more. In certain applications optical pulses are used forimaging, and in some cases for distance ranging such as LiDAR, theoptical pulse rates can range from 1K to 1M or more pulses per second.And in some cases can detect at 10M-100M or more pulses per second. Therise time of the APO/SPAD can range from pico seconds or less to 300pico seconds, and in some cases from 1 pico second to 100 pico seconds,and in some cases from 10 pico seconds to 50 pico seconds. Gain ormultiplication factor can range from 100-1000 or more, and in some casesfrom 1000 to 1,000,000 or more, in some cases the gain or multiplicationfactor can range from 3 to 1000 or more, and in some cases from 500 to5000 or more.

In some cases the Ge/GeSi 2310 can be grown on the Si layer, and Ge/GeSistrips can be formed by etching away the Ge/GeSi to the Si layer. Insome cases, a low temperature Ge/GeSi buffer layer can be formed on theSi layer prior to the Ge/GeSi growth.

In some cases, multiple wells of P or N can be formed in addition to thewells shown in FIG. 23A.

FIG. 23B shows a simple partial cross-section schematic similar to FIG.23A but without the P wells in the Si.

FIG. 24A shows a partial simplified cross-section schematic similar toFIG. 23A with microstructure holes in the Ge/GeSi. Microstructure holes2412 can be etched into the Ge/GeSi layer or region 2410 with diameterranging from 600 nm-1800 nm, and with spacing ranging from 0 nm-300 nmor more, and in some cases from 0 nm-1000 nm. The spacing of themicrostructure holes 2412 can be different for different directions forexample along the length of the strip the spacing can be 0 nm (touching)and along the width of the strip the spacing can be 300 nm-600 nm. Inthe case where the microstructure holes are touching, the holes can beinverted pyramids or conical shapes. The depth of the microstructureholes in the Ge/GeSi 2410 can be partially into the Ge/GeSi and in somecases through the Ge/GeSi to the Si layer.

FIG. 248 is similar to FIG. 24A without the P wells in the Si.

FIG. 25A is similar to FIG. 23A with the exception that Ge/GeSi 2510 isgrown in a recessed trench of the Si 2508 such that the Ge/GeSi 2510 ispredominately buried in a trench in Si 2508 using selective area growthfor example. The surface can be planarized using methods such aschemical mechanical polishing. p+ well can be formed in the Ge/GeSi andP and N+ wells can be formed in the Si. M1 can form an ohmic contact tothe p+(anode) and M2 can form an ohmic contact to the N+(cathode) and areverse bias is applied between M1 and M2.

Reference Zhu et al, Waveguided Ge/Si Avalanche Photodiode With SeparateVertical SEG-Ge Absorption, Lateral Si Charge, and MultiplicationConfiguration, IEEE Electron Device Letters, Vol. 30, No. 9, September2009; discusses Ge on Si APO in waveguide mode. In this patentspecification all the photodetectors are top surface and/or bottomsurface illuminated.

FIG. 258 is similar to FIG. 25A without the P well in Si 2508.

FIG. 26A is similar to FIG. 25A with the addition of microstructureholes 2612 in the Ge/GeSi. The microstructure holes are similar to thosediscussed in FIG. 24A.

FIG. 268 is similar to FIG. 26A without the P well in Si 2508. ReferenceKang et al, Monolithic germanium/silicon avalanche photodiodes with 340GHz gain-bandwidth product, Nature Photonics 7 Dec. 2008, DOI:10.1038/NPHOTON.2008.247 discusses a surface illuminated Ge on Si APO.Reference Martinez et al, Single photon detection in a waveguide-coupledGe-on-Si lateral avalanche photodiode, Optics Express, Vol. 25, No. 1410, July 2017, discusses waveguide coupled lateral APO structure.

Photodetectors with microstructure holes can have a higher externalquantum efficiency (EQE) than a comparable photodetector withoutmicrostructure holes. The photodetector can be a PD or APO or SPAD usedfor datacom or LiDAR or imaging. The photodetectors with microstructureholes can have EQE ranging from 2× to 10× or more than the EQE of acomparable photodetector without holes.

FIGS. 27A-B show a schematic cross-section and top view of Ge strips onSi with and without microstructure holes for use in FDTD simulation ofoptical absorption in the Ge strips. The FDTD simulation results areshown in FIGS. 28 and 29. The width of the Ge strips is 3600 nm and thegap between the strips is 400 nm, and the thickness of the Ge strips is800 nm. The length of the strip is infinite for simulation purposes. Forthe FTDT simulation all the strips either have no microstructure holes2712 or all the strips have microstructure holes. The microstructurehole diameter for the simulation is 1200 nm and the period is 1600 nm ina square lattice. The holes are circular and cylindrical. The depth ofthe microstructure holes are 400 nm and 800 nm.

FIG. 28 shows a FDTD simulation of absorption of Ge strips on Si withoutmicrostructure holes vs wavelength from 1 to 1.6 microns. The simulationaverages over +/−10 degrees from normal incidence of the optical signaland averages over polarization. The absorption which is directlyproportional to EQE is 40% or less in the wavelength range 1-1.6microns.

FIG. 29 shows FDTD simulation of optical absorption in Ge strips on Siwith microstructure holes vs wavelength from 1 to 1.6 microns. Thesimulation averages the angle of the incident photon over angle +/−10degrees from normal and by the two orthogonal polarization with 1polarization along the length of the Ge strip and another polarizationalong the width of the Ge strip. The dotted curve 2912 is for the caseof holes that are etched to a depth of 400 nm. And the solid curve 2910is for the case of microstructure holes that are etched through the Gelayer to a depth of 800 nm. The absorption ranges from 60-80% or more inthe wavelength range from 1 to 1.6 microns. The EQE is directlyproportional to absorption.

The EQE of photodetectors with microstructure holes can be higher thanthe EOE of photodetectors without microstructure holes at certainwavelengths. Ge strips on Si with microstructure hole diameter is 1200nm, the period is 1600 nm in a square lattice with cylindricalcross-section, and with an etch depth of 400 nm and 800 nm in Ge.

FIGS. 30A-B are simplified partial schematic top views of asemiconductor surface having holes configured as trenches, according tosome embodiments. The semiconductor 3010 and 3008 can be: Si, Ge, GeSiand/or 111-V material such as InP, GaAs, GaN to name a few. In this casethe microstructure “holes” are “connected” to form trenches 3060 and3062. The microstructure hole/trenches 3060 and 3062 are furtherconfigured to crisscross the surface of the semiconductors 3010 and3008, respectively. Although the trench-shaped holes in FIGS. 30A-B areshown in straight lines, they could alternatively be formed in curvedlines or a combination of straight and curved lines. The width of eachtrench is approximately one wavelength, and in some cases can be lessthan a wavelength, and in some cases can be more than a wavelength, andin some cases can have width ranging from 600 nm to 1600 nm, and can runthe length of the photosensitive area. The depth of the trench can rangefrom 100 nm to 1000 nm or more, and in some cases 50 nm to 300 nm. Thespacing of the trench can range from 100 nm to 1000 nm or more, and insome cases 100 nm-600 nm.

FIGS. 31A-B shows simplified partial cross-section schematics of a SPADor APO or PD Si photodetector for imaging and LiDAR applications,according to some embodiments. The photodetector/APO/SPAD can representa single pixel of a high-density array of PD/APO/SPAD fabricated in Siwith or without a BOX layer and monolithically integrated withCMOS/BiCMOS ASICs. In a P type Si a N well 3106 is formed followed by Pwells 3130 and 3132 and a p+ shallow well 3140 as shown. The anode 3120is formed on the P region, and the cathode 3122 is also formed on a Pregion 3142 as shown in FIG. 31A. The structure is a PNP photodetectorand a reverse bias is applied between the anode and cathode. In somecases, the cathode 3122 can be formed on the N region 3106. In somecases, the structure can be a PN, and in some cases it can be NPN, andin some cases it can be a P lowdope Nor P N, and in some cases the P andN can be interchanged. Microstructure holes 3112 such as invertedpyramids can be formed with hole dimension ranging from 400 nm to 1200nm, and in some cases 600 nm-1000 nm, and in some cases 700-1200 nm, andin some cases more than 1200 nm. Cylindrical holes can also be formed,and in some cases funnel holes, and in some cases conical holes. Theholes can be square, rectangular, polygonal, amoebic to name a few. Thespacing of the holes can range from 50 nm to 600 nm, and in some cases100 nm-1000 nm, and in some cases 50 nm-300 nm. The depth of the holescan range from 50 nm to 1000 nm or more, and in some cases 100 nm-500nm, and in some cases 50 nm-800 nm. The microstructure holes can beperiodic, and/or aperiodic and/or random. In the case of periodicmicrostructure holes it can have a square or hexagonal lattice. Opticalsignal or light reflected from objects can have wavelength ranging from700 nm to 990 nm, and in some cases from 700 nm to 1050 nm. Not shownare passivation layers in the microstructure holes, and in some casesthe microstructure holes can be filled with a dielectric layer. Also notshown are the integrated CMOS/BiCMOS ASICs and connecting transmissionlines from the PD/ADP/SPAD to CMOS/BiCMOS electronics. The EQE ofPD/ADP/SPAD with microstructure holes can be higher than a comparableEQE of PD/ADP/SPAD without microstructure holes. In reference Niclass etal, A 0.18 um CMOS Single-Photon Sensor for Coaxial Laser Rangefinders,IEEE Asian Solid-State Circuits Conference, Nov. 8-10, 2010 FIG. 1 showsSPAD micro pixel that can be integrated with CMOS electronics. ReferenceNiclass 2 et al, A 0.18-um CMOS Soc for a 100-m-Range 10-Frame/s200×96-Pixel Time-of-Flight Depth Sensor, IEEE Journal of Solid-StateCircuits, VOL. 49, NO. 1 Jan. 2014. Reference Niclass 3 et al, A 100-mRange 10-Frame/s 340×96-Pixel Time-of-Flight Depth Sensor in 0.18 umCMOS, IEEE Journal of Solid State Circuits, VOL. 48, NO. 2, February2013. Reference Ito et al, Small Imaging Depth LIDAR and DCNN-BasedLocalization for Automated Guided Vehicle, Sensors 2018, 18, 177;doi:10.3390/s18010177. Reference Villa et al, CMOS Imager With 1024SPADs and TDCs for Single-Photon Timing and 3-D Time-of-Flight, IEEEJournal of Selected Topics in Quantum Electronics, VOL. 20, NO. 6November/December 2014.

With the addition of microstructure holes in the CMOS SPAD imagers ofstructures as illustrated in FIGS. 31A-B, the EQE at 870 nm, 905 nm, 940nm wavelength can be 2×-10× or more higher than a comparable CMOS SPADimager without microstructure holes. The increase in EQE withmicrostructure holes in CMOS imager can apply to PD/APO in addition toSPAD CMOS imagers.

FIG. 31B is similar to FIG. 31A with the exception that themicrostructure holes 3112 are first etched followed by a shallowdiffusion of p+ dopants such as Boron to form shallow P well 3144.

FIGS. 32A-B shows partial simplified cross-section schematics similar toFIG. 31B with the addition of a Ge/GeSi layer on top of the N well. TheGe/GeSi 3208 can be I or low dope P, and in some cases N withmicrostructure holes 3212 etched in the Ge/GeSi 3208. A p+ layer 3240can be grown over the top surface following the contour of themicrostructure holes 3212, and in some cases the p+ layer 3240 or regioncan be diffused with P type ions such as boron. In some cases, thep+3240 can be polycrystalline Si, and in some cases p+ amorphous Si. Theanode electrode 3220 can be formed on the p+ layer 3240, and the cathode3222 can be formed on the N well 3206. A reverse bias is applied betweenthe anode and cathode. The BOX layer in some cases can be optional. Thephotodetector can be PD/APO/SPAD and can be a high density 2D array forimaging LiDAR applications, and can be monolithically integratedCMOS/BiCMOS ASICs. As shown the structure is a PIN and in some cases canbe PN, and in some cases can be PNP, and in some cases can be NP, and insome cases NPN, and in some cases PINP, and in some cases NIPN. Otherdoped regions including graded doped regions can be included. Light oroptical signal can impinge from the top surface, and in some cases fromthe bottom substrate surface. Wavelength for detection can range from800 nm to 1800 nm, and in some cases 800 nm-1550 nm, and in some cases900 nm-1000 nm, and in some cases 900 nm-1550 nm. The thickness of the Nwell can range from 100 nm to 2000 nm or more, and in some cases can beless than 100 nm.

The microstructure holes 3212 can have a lateral surface dimensionranging from 500 nm to 1600 nm. The spacing between the microstructureholes can range from 50 nm to 800 nm. In some cases, the spacing can bemore than 800 nm. In some cases, with conical holes the spacing can be 0nm and in some cases can be intersecting. The depth of themicrostructure holes can range from 100 nm to 1000 nm and in some casesgreater than 1000 nm.

The Ge/GeSi layer 3206 can have a thickness ranging from 100 nm-1000 nm,and in some cases greater than 1000 nm. The Ge/GeSi can be selectivearea grown on the Si N well, with or without a low temperature bufferlayer of Ge/GeSi, and in some cases the Ge/GeSi can be strain or in somecases can be no strain.

In some applications microstructure holes 3212 may not be necessary inthe Ge, however photodetectors with microstructure holes can have ahigher EQE or responsivity at certain wavelengths than a comparablephotodetector without microstructure holes. The rise time of thisphotodetector structure can be in the 10s of pico seconds or less andcan provide high depth resolutions in lidar applications. The number ofpulses per second can range from 1K-1M, and in some cases greater than1M.

For optical data communication using the new structures described inthis patent specification, the data rate can range from 1 Gb/s-25 Gb/s,and in some cases 25 Gb/s-50 Gb/s, and in some cases greater than 50Gb/s. For structures such as illustrated in FIGS. 32A-B xxsy, PAM4 canincrease the data rate further by 2×, see reference Kerrebrouck et al,High-Speed PAM4-Based Optical SOM Interconnects With Directly ModulatedLong-Wavelength VCSEL, Journal of Lightwave Technology, DOI10.1109/JLT.2018.2875538

FIG. 32B is similar to FIG. 32A with the exception of a p+ layer 3242formed on the Ge/GeSi layer 3208 prior to etching microstructure holes3212.

The microstructure holes 3212 can be passivated with amorphoussemiconductor and/or dielectric, and in some cases the microstructurehole can be filled with dielectric.

In some cases of structures such as illustrated in FIGS. 23A-B, 24A-B,25A-B26A-B, and 32A-B for example, balanced photodetector (PD/APO/SPAD)can be used to further reduce noise; for example see references Wang etal, InP-based Balanced Photodiodes Heterogeneously Integrated on SOINano-Waveguides, IEEE 976-1-5090-1602-0/16; Runge et al, WaveguideIntegrated Balanced Photodetectors for Coherent Receivers, IEEE Journalof Selected Topics in Quantum Electronics, Vol. 24, No. 2 March/April2018; Islam et al, Distributed Balanced Photodetectors for Broad-BandNoise Suppression, IEEE Transactions on Microwave Theory and Techniques,Vol. 47, No. 7 Jul. 1999. Microstructure holes can be included on thebalanced photodetectors to enhance the EQE at certain wavelengths. Seealso reference; Zheng et. al, Fluidic Hetergeneous

Microsystems Assembly and Packaging, Journal of MicroelectromechanicalSystems, Vol. 15, No. 4, August 2006. See also reference, Park et. al, AFirst Implementation of an Automated Reel-to-Reel Fluidic Self-AssemblyMachine, https://doi.org/10.1002/adma.201401573, Jun. 27, 2014.

FIGS. 33A-C show simplified partial schematic cross-sections ofmicrostructure holes formed on semiconductor surfaces, according to someembodiments. Holes 3312 formed in semiconductor material 3302 in FIG.33A can have conical or inverted pyramid shapes. The holes 3312 can bespaced by a finite distance for example 50 nm to 1000 nm as shown. Holes3314 of FIG. 33B illustrate that in some cases, the conical or invertedpyramid microstructure holes can touch. Holes 3316 of FIG. 33Cillustrate that in some cases, the conical or inverted pyramidalmicrostructure holes can intersect.

In some cases, the microstructure holes on the surface of aphotodetector to enhance EQE can include a combination of all 3 casesshown in FIGS. 33A-C. The holes can be passivated with dielectrics orwith semiconductor that can be crystalline, polycrystalline, and/oramorphous and can be a semiconductor that is different than thesemiconductor on which the microstructure holes are formed. In somecases, the microstructure holes can be partially or entirely filled witha dielectric.

The use of microstructure holes to enhance EQE of structures such asillustrated in FIGS. 33A-C can be applied to material other thansemiconductor, for example polymers, graphene to name a few. In somecases, reverse bias is applied to generate an electric field to sweepout photo generated carriers. In some cases, a forward bias can bebiased also to generate an electric field to sweep out photo generatedcarriers.

The EQE of photodetectors under reverse or forward bias withmicrostructure holes in all new structures described in this patentspecification can be greater than the EQE of a comparable photodetectorunder reverse or forward bias at certain wavelength.

FIG. 34A shows a known optical module. For further details of theexample shown see: IBM ref. Doany, High Density Optical Interconnectsfor High Performance Computing, O F C 2014 M3G1. The module consists offour separate components. FIG. 34B shows a condensed optical module,according to some embodiments of this patent specification. In thiscase, the separate components in the known example shown in FIG. 34A are“condensed” to a single component 3400. In particular, three of thecomponents are monolithically integrated: (1) the photodetector array;(2) the CMOS/BiCMOS ASICs for driving the Vertical Cavity SurfaceEmitting Laser (VCSEL) array; and (3) the ASICs for amplifying andconditioning and/or processing the electrical signal from thePhotodetector array. The fourth component, the VCSEL array, can beattached to the monolithically integrated Photodetector array andCMOS/BiCMOS ASICs using fluidic self-assembly, robotic assembly, Van DerWaals epitaxial lift off attachment, wafer bonding, hetero epitaxial toname a few. The electrodes of the VCSEL array can be attached to thetransmission line of the CMOS/BiCMOS driver using a back end of the lineprocess. This reduction in component parts can be a significantreduction in cost. As shown in FIG. 34B the single component 3400 can bedirectly attached to the PCB, motherboard, Pin Gate Array connectors(PGA). The aggregated data rate can be over 400 Gb/s with a 4×12 arrayof VCSELs and Photodetectors, where each channel can be 10 Gb/s or more.

For further details of a High density VCSEL array and detector arraywith 48 channels for onboard optical module, see reference Doany et al,Terabit/Sec VCSEL-Based 48-Channel Optical Module Based on Holey CMOSTransceiver IC, Journal Of Lightwave Technology, Vol. 31, No. 4, Feb.15, 2013.

FIG. 35A shows a known onboard optical module. The optical moduleconsists of six components, namely, the interposer, organic substrate,VCSEL driver, Trans-impedance Amplifier (TIA), VCSEL array, andPhotodetector (PD) array. The module is attached directly to themotherboard/PCB. See, Ref, Nasu et al, >1.3 Tb/s VCSEL-Based On-BoardParallel-Optical Transceiver Module for High-Density OpticalInterconnects, Journal of Lightwave Technology, Vol. 31, No. XX January,2018. FIG. 35B shows an optical module according to some embodiments ofthis patent specification. In this example, the six components arereduced to a single component. The Photodetector array can be Si, GeSi,Ge on Si and is monolithically integrated with CMOS/BiCMOS ASICs, whichinclude the laser driver and the TIA and other electronics forprocessing, conditioning and communication for the laser and thePhotodetector arrays. The aggregated data rate for a 24 channel can beover 600 Gb/s where each channel can have a data rate of 25 Gb/s-28Gb/s. The VCSEL array can be attached to the monolithically integratedchip at the wafer scale level using fluidic self-assembly, roboticassembly or other wafer scale assembly, and the electrodes of the VCSELarray can be attached the transmission line of the laser driver ASICsusing a back end of the line process. This reduction in componentsgreatly reduces packaging complexity and therefore the cost of theon-board optical module.

Monolithic integration of high density photo-sensing arrays for imagingwith CMOS ASICs with inverted pyramid holes on the surface of thesensing absorption layer have shown extension of the optical sensitivityto 1000 nm wavelength, see for example Ref, Yokogawa et al, IRsensitivity enhancement of CMOS Image Sensor with diffractive lighttrapping pixels, Scientific Reports 7:3832 DOI:10.1038s41598-017-04200-y. The CMOS image sensor operates at very lowframes per second, typically in the millisecond range or longer. Inaddition, reference Yokogawa shows the inverted pyramid array on thesurface of the absorption of the photo sensor without indications ofapplying external bias voltage for example reverse bias. The photosensing may depend only on diffusing of photo carriers generated tocollecting electrodes in a CMOS transistor.

With monolithic integration of PD/APO/SPAD arrays with CMOS/BiCMOSelectronics in structures such as illustrated in FIG. 35B, the arraysize can be greater than 48 channels and in some cases the array sizecan be greater than 100 channels, and in some cases the array size canbe greater than 1000 channels. The data rate for each channel can rangefrom 10 Gb/s-25 Gb/s or more. By monolithically integrating, parasiticsdue to connecting the channel or PD/APO/SPAD to the electronics can besignificantly lowered compared to wire bonding or soldier bumptechnology that may be required to attach the transmission lines of adetector array chip that is not integrated monolithically with theelectronics. The parasitics can consist of capacitance, inductance,and/or resistance.

FIGS. 36A-B show simplified partial schematic top views of aninterdigitated photodiode and elongated microstructure holes, accordingto some embodiments. The interdigits can be in two orthogonalorientations and the microstructure holes or islands can be elongatedalong the direction of the interdigit electrodes. In some cases themicrostructure hole or island can be rectangular (holes 3212 in FIG.36A), oval (holes 3214 in FIG. 36B), and/or polygonal to name a few. Inthe cases where the holes are elongated along the direction of theinterdigit electrodes, the interdigit electrode spacing can be narrowerfor example less than 1000 nm. The dimension of the rectangular hole orisland can range from 100 nm-1500 nm or more. For example, the narrowdimension of the rectangular hole can have dimensions ranging from 50nm-1000 nm, and in the long direction the dimension can range from 400nm-2000 nm or more.

In some cases of structures such as illustrated in FIGS. 36A-B, thespacing between the interdigit electrodes or p and n junctions can rangefrom 100 nm to 1000 nm or more. The width of the electrode or p and njunctions can range from nm to 500 nm. M1 (3620) and/or M2 (3622)interdigit electrodes can form Schottky, metal oxide semiconductorand/or ohmic to semiconductor and/or ohmic to p and/or n junctions.

Data rates of structures such as illustrated in FIGS. 36A-B and theother new structures described in this patent specification can rangefrom 1 to 50 Gb/s or more and in some cases 10 to 30 Gb/s. In some casesthe rise time (10-90% of pulse amplitude) can range from 1 to 100 psecand in some cases 10 to 50 psec and in some cases 100 psec to 10 nsec.

In structures such as illustrated in FIGS. 36A-B and the other newstructures described in this patent specification, arrays ofphotodetector, PD/APD/SPAD, can have 4 to 1000 photodetectorsor more andin some cases tens of thousands to millions of photodetectorsmonolithically integrated with CMOS or BiCMOS ASICs and electricallyconnected to the ASICs operating in a reverse bias in the cases with pand/or n junctions and in the cases with Schottky and/or MOS junctionsthe photodetector can operate in the reverse and/or forward bias. In thecase of ohmic junctions to the semiconductor, bias can be either forwardor reverse.

Lateral dimension of the photosensitive region of structures such asillustrated in FIGS. 36A-B and the other new microhole structuresdescribed in this patent specification can range from one micron tothousands of microns and in some cases more than one thousand microns.

FIG. 368 is similar to FIG. 36A except that the microstructure holes3214 are oval shaped. Note that in some cases the hole can have othershapes such as diamond shaped holes. Note that in all such cases, onelateral dimension is larger than the orthogonal dimension. The ovalshaped holes allow the electrodes to be closely spaced; for example theelectrode spacing can range from 200 nm-1000 nm and in some cases from200 nm-500 nm for high data rates, for example 20 Gb/s or more. Twolateral dimensions of the elongated holes can range from 100 nm-1500 nm,and in some cases 1 lateral dimension can range from 100 nm-1000 nm, andthe second lateral dimension can range from 500 nm-2000 nm, and in somecases the first lateral dimension can range from 300 nm-500 nm, and thesecond lateral dimension can range from 500 nm-1500 nm.

FIG. 37 shows current voltage characteristics “IV” of a metal oxidesemiconductor junction under both M1 and M2 electrodes of aninterdigitated photodiode, according to some embodiments. The dashed IVcurve shows a sharp breakdown at approximately 2.5 volts in either thereverse or forward voltage bias. This breakdown may be Zener breakdownwhich is due to tunneling through the oxide layer and can be controlledby the intensity of the absorbed photon in the semiconductor. Theabsorbed photon can cause a change in the number of minority carriers inthe semiconductor which can affect the Zener breakdown voltage. ThisZener breakdown can result in a responsivity at 850 nm of 7 A/W or more.Three types of gain can be observed in interdigitated metalsemiconductor metal photodiodes, Zener gain, photoconductivity gain andavalanche gain.

FIGS. 38A-C illustrate an FDTD simulation of a structure, according tosome embodiments. The structure is shown in FIG. 38C, where a GeSi layerwith varying concentration of Ge ranging from 10%-30% has a thickness of1000 nm grown on Si device layer of 200 nm on top of a BOX layer of 2000nm on Si substrate. The microstructure holes 3812 have a diameter of 700nm and a period of 1000 nm in a hexagonal lattice, and light impinge onthe surface of the GeSi layer. The optical signal is averaged over anangle of +/−10 degrees from normal incidence. FIG. 38A shows the FDTDsimulation with Ge concentration of 10, 20, percent in GeSi withmicrostructure holes. The vertical axis is absorption of the photons,and the horizontal axis is wavelength. The absorption is directlyproportional to the external quantum efficiency. The solid curve 3820shows absorption of GeSi with 10% Ge, the dashed curve 3222 showsabsorption of GeSi with 20% Ge, and the dotted curve 3224 showsabsorption of GeSi with 30% Ge.

FIG. 38B shows FDTD simulation of the optical field of a similarstructure as in FIG. 38C but without microstructure holes, and with Geconcentration of 10 percent (curve 3830), 20 percent (curve 3832) and 30percent (curve 3834) in GeSi. As can be seen the absorption or externalquantum efficiency of a structure with microstructure holes can havehigher absorption than a similar structure without microstructure holesat certain wavelengths.

With the addition of Ge in GexSh-x where x can range from 0.05 to 1where 1 in pure Ge, the wavelength of the GeSi can be extended beyond1000 nm as shown in FIG. 38a . With x=0.1 to 0.3 in GexSh-x theabsorption in structures such as illustrated in FIGS. 38A-C and theother GeSi microhole new structures described in this patentspecification which is directly proportional to the EOE can be greaterthan 50% from 800-1200 nm wavelength, and in some cases to 1350 nm.Photodetector PD/APO/SPAD comprising GeSi can be monolithicallyintegrated with CMOS/BiCMOS ASICs. In some optical data centerinterconnect (DCI) applications the wavelength can range from 950nm-1080 nm; for example see reference, Simpanen et al, Long-Reach 1060nm VCSEL-SMF Optical Interconnects, DOI: 10.1109/ECOC.2018.8535524.Where 1060 nm was used for long reach (2 Km) optical data communication.

FIGS. 39A-C show partial simplified cross-section schematics ofinterdigitated Ge/GeSi on Si photodiode, according to some embodiments.In some cases the interdigitated Ge/GeSi on Si photodiode can be avertical structure Ge/GeSi on Si photodiode with anodes and cathodes.For example, M2 can be cathode, and M1 can be anode. In the structureshown in FIG. 39A, microlens 3930 is formed on the bottom of the Sisurface. Not shown are anti reflection coatings that can be applied tothe micro lens. Light or optical signal impinge from the bottom surface,and the micro lens focus the light to the photodiode. The Ge/GeSi can beI or low doped grown on Si with or without a buffer layer. On top of theI or low dope Ge/GeSi a p+ Ge/GeSi or polySi can be formed. The I or lowdope Ge/GeSi can have thickness ranging from 100-1000 nm or more, andthe p+ Ge/GeSi or polySi can have a thickness range of 50 nm-500 nm ormore. N+ well can be formed in the Si which can be I or low dope P or NSi. Microstructure holes 3912 can be formed partially into the p+region, though the p+ region into the I or low dope Ge/GeSi region, orthrough the p+ region and through the I or low dope Ge/GeSi region tothe Si. Cathode or M2 can be formed on the N+ well, and anode or M1 canbe formed on the p+ region. A reverse bias is applied between the anodeor M1 and cathode or M2. Arrays of this photodiode can be fabricated andmonolithically integrated with CMOS/BiCMOS ASICs on a single Si chip.The number of photodetectors in the array can range from 4-over 1000,and in some cases in the 100,000 range, and in some cases in the1,000,000s range. Wavelength range from 1000 nm-1800 nm.

FIG. 398 is similar to FIG. 39A with the exception that the Ge/GeSiregion has pyramid “holes” 3914 composed of Si. Since Si has a loweroptical index of refraction than Ge/GeSi and light is illuminated on theback surface the Si pyramids appears to be holes that are filled withSi, as in earlier examples microstructure holes can be filled withdielectrics such as Si dioxide for example.

FIG. 39C is similar to FIG. 39A where the microstructure holes 3916,3917 and 3918 are etched to the Si region and in some cases etched intothe Si region (3917), and in some cases etched to the Si followed by awet etch to form an inverted pyramid (3918). The holes can be circular,rectangular, square, polygonal, oval, amoebic and/or any combination ofshapes. In some cases, the holes can be cylindrical, funnel,trapezoidal, pyramidal, or inverted pyramidal.

The microstructure holes in structures such as illustrated in FIGS.39A-E can have lateral dimensions ranging from 100 nm-2500 nm and insome cases from 500 nm-1200 nm, and in some cases from 600 nm-1200 nm,and in some cases more than 1200 nm. The spacing between the holes canrange from 0 nm “touching or overlapping” to 1000 nm, and in some cases100 nm-2000 nm, and in some cases 300 nm-600 nm, and in some cases morethan 1000 nm. The holes can be periodic, and/or aperiodic, and/orrandom, and/or any combination of periodic, aperiodic, and/or random.

A reverse bias can be applied between the P anode and the N cathode ofstructures such as illustrated in FIGS. 39A-E, with reverse biasvoltages ranging from −1 volt to −35 volts or more, and in some casesfrom −1 volt to −4 volts. Not shown are transmission lines connectingthe anode and cathode to the CMOS/BiCMOS ASICs. High density array canbe formed comprising of PD/APO/SPAD. The array size can range from 4 to100 or more, and in some cases to 1000 or more, and in some cases totens to hundred thousands or more, and in some cases to millions.

FIG. 390 shows a simple cross-section of Ge on Si pyramids used for FDTDsimulation. The Si pyramids 3914 are formed on Si substrate 3902 with abase side dimension of 750 nm, a period of 1000 nm in a square lattice.The Ge layer grown on top of the Si pyramids is 1 micron thick. Lightand/or optical signal is illuminated from the bottom surface where thebottom surface has an anti-reflection coating.

FIG. 39E shows the FDTD simulation of the optical signal from 1200 nm to1450 nm wavelength and where the vertical axis is the enhancedabsorption, As can be seen the dotted curve 3910 shows enhancedabsorption greater than 50% over the wavelength range. The EQE isdirectly proportional to the absorption and can have an EQE of 50% ormore over this wavelength range at certain wavelengths, and in somecases 30% or more EQE at certain wavelengths, and in some cases 20% ormore EQE at certain wavelengths.

FIG. 40 shows a simplified partial cross-section of a monolithicintegrated Photodetector array with CMOS/BiCMOS ASICs, according to someembodiments. The Photodetector in the array can be photodiode and/oravalanche photodiode, and/or single photon avalanche photodiode. Theabsorption layer of the Photodetector can be Ge/GeSi with Geconcentration ranging from 1% to 100% where 100% represents pure Ge, andin some cases the Ge concentration can be 10%-30%, and in some cases theGe concentration can be 10%-60%. Micro lenses 4050 as in FIG. 39A-D areformed on the bottom surface of the Si 4000 to focus the light and/oroptical signal into the Photodetector. The number of elements in aPhotodetector array 4010 can range from 1 to 1,000,000 or more, and insome cases 12-96, and in some cases 24-96, and in some cases 100-1000,and in some cases tens of thousands, and in some cases hundreds ofthousands, and in some cases in the millions. The photodetectors in thearray can be electrically connected to the CMOS/BiCMOS ASICs and a biasvoltage is applied to the Photodetectors. In some cases, the biasvoltage is reverse bias, and in some cases the bias voltage can beforward biased in cases where the IV characteristics are approximatelysymmetric. In addition, CMOS/BiCMOS ASICs can be monolithicallyintegrated to drive the VCSEL array. The CMOS/BiCMOS electronics fordriving the VCSEL array can also have ASICs for signal processing,and/or waveform conditioning for optimal data transmission. The VCSELarray can be assembled on the back surface of the Si substrate usingself-assembly such as fluidic self-assembly, robotic assembly, and/orany other assembly methods. Electrodes 4030 connect the CMOS/BiCMOSlaser transmitter, laser driver, and ASICs, can be formed to connect thelaser array using back end of line process. The VCSEL array can havemicro lenses 4052 formed to focus the light to a similar micro lens thatsubsequently focus the light into parallel optic fiber ribbons 4020. Themicro lens 4052 of the VCSEL array, and the micro lens 4050 for thePhotodetector array can be tele-centric with the collecting micro lensthat are used to connect to the optical fiber ribbons. The Si chip 4000containing both the VCSEL array, the Photodetector array, CMOS/BiCMOSelectronics can be mounted directly on a printed circuit board (PCB)using technologies such as soldier bumps 4032. Each channel can havedata rates ranging from 1-25 Gb/s or more.

Wavelength can range from 990 nm-1800 nm. In some cases, the VCSEL arraycan be assembled on the top surface as in FIG. 35. Also shown in FIG. 40is transmitting optical signal 4040, receiving optical signal 4042.

Coupling between micro lens using telecentric lens design can increasetolerance due to optical misalignment of structures such as illustratedin FIG. 40. See for example reference, Kuo et al, Free-space opticallinks for board-to-board interconnects, Applied Physics A MaterialsScience & Processing, DOI: 10.1007/s00339-009-5144-z.

Wavelength at 1060 nm VCSEL or laser can be used for short reach opticaldatacenter interconnect applications, see for example reference; Herouxet. al, Energy-Efficient 1060-nm Optical Link Operating up to 28 Gb/s,Journal of Lightwave Technology, Vol. 33, No. 4, Feb. 15, 2015. See alsoreference; Heroux et. al, Low power CMOS-driven 1060 nm multimodeoptical link, OFC 2014. See also reference, Doany, High Density OpticalInterconnects for High Performance Computing, OFC 2014.

FIGS. 41A-C show simplified views of pits etched on a Si surfaceconfigured for fluidic self-assembly, according to some embodiments.FIG. 41A shows a 3D view of a rectangular pit etched on the Si surface4110 for fluidic self-assembly. One or more side of the pit 4130 canhave corrugations for example rectangular slots 4120 extending on theside wall of the pit partially and/or entirely from the surface to thebottom of the pit. As shown two of the side walls have slots etched intothe side walls.

FIG. 41B shows a simplified partial top view of the rectangular pit 4130etched into the surface of the Si 4110 for fluidic self-assembly andshowing the slots 4120 etched into two of the side walls of therectangular pit 4130. A surface emitting laser array chip 4110 is alsoshown fluidic assembled in the rectangular pit. The fluid in the slotcan be heated such that the expansion of the fluid in the slots can pushthe laser array chip to the bottom right corner of the rectangular pit.This allows precision alignment of the optical components to micro lensassembly that couple the light from the VCSEL array that can haveintegrated micro lenses to external fiber ribbon. Not shown areelectrical connections to the VCSEL array that can be made back end ofline process. Also not shown are trans silicon vias (TSV) that can beused to connect the bottom of the VCSEL array to CMOS/BiCMOS ASICs. Oncethe VCSEL array chip is in position, and most or all the fluids haveevaporated additional heat can be applied to solder the laser array tobottom electrodes using technology such as solder bump technology. Thewidth of the slot can range from 1-100 microns or more, and the depth ofthe slot can range from 1-100 microns or more. The length of the slotcan range from 1-100 microns or more.

FIG. 41C shows a simplified partial top view of a polygonal pit havingfive sides. Three of the five sides are etched with slots 4122. A VCSELor laser array also polygonal with five sides 4134 is shown that can fitinto the pit in only one orientation. The fluid in the slots 4122 canexpand with temperature and can push the polygon shaped laser array chipto the bottom left corner for precision optical and electricalalignments. Not shown are tabs that can be formed on the surface of thelaser array chip that can prevent the laser array chip from falling intothe pit upside down for example. Not shown are the transmission linesthat can be attached to the laser array to the CMOS BiCMOS ASIC laserdriver and other signal conditional and/or processing electronics. Theadvantage of slotting the side of the pit can increase the fluid volumethat can expand with temperature, and can therefore act to position thelaser array chip towards a predetermined corner that can allow precisionoptical and electrical alignments.

FIGS. 42A-B and 43A-B are partial simplified cross-sections of a Ge/GeSion Si photodiode, according to some embodiments. The Ge/GeSi on Siphotodiode can be interdigitated with M1 and M2 electrodes where M1 canbe the anode, and M2 can be the cathode. The Ge/GeSi layer is a graded Ptype doped layer with doping at the higher level at the surface comparedto the doping level at the Ge/GeSi interface with n Si. Microstructureholes 4212 can be formed in the Ge/GeSi and in some cases can extendinto the n Si. N+ wells are formed in then Si. The wavelength of theoptical signal that can impinge on the top surface and in some cases canimpinge from the bottom surface range from 990 nm-1600 nm, and in somecases 1000 nm to 1350 nm. The photons are absorbed predominately in theGe/GeSi region/layer and with a reverse bias between the anode andcathode the photo carriers are predominately electrons that are sweptfrom the P type Ge/GeSi toward the N+ Si cathode. Such a device can becalled a unitary traveling carrier “UTC” photodiode. Such UTCphotodiodes can have higher speed and/or data rate than photodiodes thathave bi-polar carriers, see for example ref. Piels et al, 40 GHz Si/Geuni-traveling carrier waveguide photodiode, DOI10.1109/JLT.2014.2310780. Journal of Lightwave Technology.

The Ge/GeSi layer in structures such as illustrated in FIGS. 42A-B and43A-B can have a thickness ranging from 200-1000 nm and in some cases500-1000 nm and in some cases more than 1000 nm. The microstructure holecan be funnel, cylindrical, trapezoidal, pyramidal, and the lateraldimension atthe surface can range from 300 nm to 1300 nm, and in somecases 600 nm-1200 nm and in some cases 800 nm-1500 nm, and in some casesgreater than 1500 nm. The depth of the holes can range from 200 nm to1000 nm, and in some cases more than 1000 nm. The spacing between themicrostructure holes can be 0 “touching or intersecting” to 600 nm, andin some cases 100 nm-800 nm, and in some cases more than 800 nm. Themicrostructure holes can be partially in the Ge/GeSi, can extend throughthe Ge/GeSi to the Si interface, and in some cases into then Si. The nSi layer can also be a low dope P or N Si layer with resistivity greaterthan Ohm-cm and in some cases greater than 25 Ohm-cm, and in some cases100-1000 or more Ohm-cm. A BOX layer can be beneath the I or low dope Silayer, and in some cases the I or low dope Si can be the substrate. Insome cases, a microlens can be formed on the bottom of the Si substrateto focus light optical signal impinging on the bottom surface andfocusing the signal to the photodector. The reverse bias applied theanode and cathode can range from −1 volt to −35 volts or more, and insome cases from −1 volt to −5 volts, and in some cases from −1 volt to−3.3 volts. The spacing between the M1 and M2 electrode can range from500 nm to 1000 nm and in some cases greater than 1000 nm and in somecases less than 500 nm. The spacing between M1 and M2 in some cases canrange from 300 nm to 3000 nm, and in some cases more than 3000 nm. Datarate can range from 1 Gb/s to 50 Gb/s and in some cases greater than 50Gb/s and in some cases less than 1 Gb/s. In some cases, the data ratecan range from 10 to 40 Gb/s. The rise time of the photodiode to animpulse response can range from 1 pico second to 100 pico seconds, andin some cases from 10 pico seconds to 100 pico seconds, and in somecases less than 30 pico seconds. The rise time can be defined as the10-90% of the leading edge of the impulse response.

FIG. 42B is similar to FIG. 42A with the addition of a p+ well on thetop surface of the Ge/GeSi to ensure a graded doping, where the dopinglevel at the surface is high, and the doping level decreases in depthtowards the Si interface. The microstructure holes 4214 are also shownas rectangular instead of conical or pyramidal.

FIG. 43A is similar to FIG. 42A with the addition of a P charged well inthe I or low dope Si. A BOX layer is included, and in some cases a BOXlayer may not be necessary. The microstructure holes 4312 can be withinthe Ge/GeSi layer and in some cases can extend into the I or low dope Siregion. A reverse bias is applied between the anode and cathode with thebias voltage ranging from −3 volts to −35 volts, and in some cases ahigher negative potential than −35 volts. Avalanche gain can range from3 dB—30 dB or more.

FIG. 43B is similar to FIG. 43A with the addition of a p+ doped well inthe Ge/GeSi layer that can be P doped or lightly P doped. Themicrostructure holes 4314 can be within the Ge/GeSi and in some casescan extend into the I or low dope Si. Optical signal can impinge on thetop surface, and in some cases can impinge from the bottom surface.

FIGS. 42A-B and FIGS. 43A-B show partial simplified cross-sectionschematics of Ge/GeSi on Si where a BOX layer can be optional and wherethe Ge/GeSi layer or region is P doped and in some cases p− doped and insome cases re doped such that when the optical signal that can impingefrom the top surface and/or from the bottom surface electron/holes aregenerated in the Ge/GeSi and where the electron is a minority carrierand is swept toward the cathode when the photodetector is under reversebias, and where the electrode on the P layer or region is the anode, andthe electrode on the N region is the cathode. The photo generatedelectron can be a uni-traveling carrier (UTC) photodetector and sinceelectrons have a higher drift velocity than holes, this UTCphotodetector can be faster than a bipolar or hole dominated carrierphotodetector; see forexample reference Piels et. al, 40 GHz Si/Geuni-traveling carrier waveguide photodiode, Journal of LightwaveTechnology, DOI 10.1109/JLT.2014.2310780.

Wavelength in structures such as illustrated in FIGS. 42A-B and FIGS.43A-B can range from 1100 nm to 1600 nm where photons are absorbedpredominately in the Ge/GeSi regions, and in some cases wavelength canrange from 900 nm to 1650 nm where photons are absorbed predominately inthe Ge/GeSi regions and in some cases for top surface illumination thewavelength range can be 800 nm-1650 nm where the photons are absorbedpredominately in the Ge/GeSi regions.

Not shown in FIGS. 42A-B and FIGS. 43A-B are the CMOS/BiCMOS ASICs thatcan be monolithically integrated with the UTC PD/APO/SPAD. An advantageof a UTC APO/SPAD is the reduction in noise since only electrons areinvolved in the ionization process.

FIGS. 44A-D, 45A-C and 46A-D show basic simplified steps for monolithicintegration of microstructure holes photodetector with CMOS and/orBiCMOS ASICs, according to some embodiments. FIG. 44A shows the startingmaterial for a CMOS process consisting of a SOI substrate with a lowdope P device layer. FIG. 44B shows the forming of deep N wells 4406 anda shallow P well 4410. The doped wells can be formed by diffusion ofdopant ions and/or by ion implantation of dopant ions. FIG. 44C showsthe formation of cathode 4422 and anode 4420 metals and/or silicide tocontact the N and P regions. FIG. 44D shows the formation ofmicrostructure holes 4412 which can be dry etched and/or wet etched. Inthe case of wet etch inverted pyramids can be formed.

Not shown in FIGS. 44A-D, 45A-C and 46A-D are isolation trenches forboth electrical and/or optical between photodeterctors and/or betweenCMOS ASICs. Also not shown are dielectric layers such as Si dioxidewhich can be deposited on the surface of the microstructure holes and/orthe electrodes. Also not shown are anti-reflection coatingsplanarization layers, transmission lines from the photodetector to theCMOS/BiCMOS ASICs, and any other layers or components to complete themonolithic integration. Trans silicon vias (TSV) can be formed toconnected electrodes, and/or any electrical contacts on the surface toelectric contacts on the bottom surface that can be directly contactedto electrodes on a printed circuit board such that an interposer may notbe necessary.

The starting point of FIGS. 45A-C is FIG. 44A. The process is similar toFIGS. 44B-D. In FIG. 45A low dope deep N well 4506 is formed followed bya highly doped shallow P well 4510. In FIG. 45B shows the formation ofcathode 4522 and anode 4520. FIG. 45C shows the formation ofmicrostructure holes 4512.

In FIG. 46A the starting material is shown. In FIG. 46B the shallow Nwell are formed in the P device layer, and shallow N well is formed onthe surface. In FIG. 46C the cathode 4622 and anode 4620 electrodes areformed on the N and P surfaces respectively, and in FIG. 46Cmicrostructure holes 4612 are formed.

FIGS. 47A-C and 48A-C show a basic simplified processing steps tomonolithically integrate interdigitated photodetector with CMOS/BiCMOSASICs, according to some embodiments. FIG. 47A shows a basic startingmaterial for CMOS/BiCMOS ASICs where SOI substrate is used and a devicelayer is a low dope P type semiconductor. FIG. 47B shows the formationof metal interdigits 4722 and 4720 on the surface of the low dope Psemiconductor. FIG. 47C shows the formation of microstructure holes 4712between the interdigitated electrodes. In this metal-semiconductor-metal(MSM) structure the biasing voltage can be either forward bias orreverse bias since the metal contact to the semiconductor can beSchottky contact or MOS contact and are back to back diodes.

The starting point of the process shown in FIGS. 48A-C is also FIG. 47A.In FIG. 48A the P and N wells are formed. In FIG. 48B the interdigitatedelectrodes are formed over the P and N wells. And in FIG. 48Cmicrostructure holes 4812 are formed.

In some cases in the structures illustrated in FIGS. 47A-C and 48A-C,Ge/GeSi layers can be grown on the p− device layer and the Ge/GeSi canalso be p− doped, and P and N wells can be formed on the Ge/GeSi and/orSi and the processing steps are similar. In some cases the BOX layer maynot be necessary. See for example FIGS. 42A-B and FIGS. 43A-B forGe/GeSi on Si photodetectors.

FIGS. 49A-F show basic fabrication steps for Ge/GeSi on Siinterdigitated photodiode that can be monolithically integrated withCMOS/BiCMOS ASICs, according to some embodiments. Arrays of theseGe/GeSi photodiodes can be monolithically integrated with CMOS/BiCMOSelectronics.

FIG. 49A shows a starting material, in this case SOI with a P devicelayer and in some cases the P device layer can be low doped or re doped.In some cases, the device layer can be N doped or low N doped and the Pand N can be interchanged. In some cases, the starting material can be alow dope or re doped Si wafer without the BOX layer.

FIG. 49B shows the growth of Ge or GeSi on Si with or without a bufferlayer, and the Ge/GeSi can be relaxed or strained. The thickness of theGe/GeSi layer can range from 200 nm to 1000 nm or more.

FIG. 49C shows etched trenches in the Ge/GeSi to the Si device layer. Insome cases, the strips of Ge/GeSi can be formed by selective area growthsuch that etching trenches is not necessary.

FIG. 49D shows the forming of p+ wells in the Ge/GeSi and the N+ wellsin the low dope P Si.

FIG. 49E shows the forming of ohmic contacts to the P and N wells andthe M1 and M2 interdigitated electrodes which in some cases can beformed in separate steps.

FIG. 49F shows the etching of microstructure holes 4912.

Not shown in FIGS. 49A-F are passivation layers that can partially orentirely cover the microstructure holes and any exposed edges of theGe/GeSi. And in some cases passivation layers can cover the surface ofthe Si and any exposed edges of the Si. Also not shown are theCMOS/BiCMOS ASICs that can be monolithically integrated, transmissionlines from the photodetector to the CMOS/BiCMOS ASICs, and anyelectrical optical isolation trenches to name a few.

FIG. 50 shows a simplified partial cross-section schematic of a Ge/GeSion Si photodiode that can be monolithically integrated with CMOS/BiCMOSASICs, according to some embodiments. The BOX layer can be optional. N+well can be diffused or ion implanted into the low dope P Si layer, anda low dope P Ge/GeSi can be grown on the N+ Si with or without a buffer.The thickness of the Ge/GeSi can range from 300 nm-1000 nm, and in somecases more than 1000 nm. A p+ well is formed on the surface of theGe/GeSi. Anode can be formed on the p+ Ge region and cathode can beformed on the N+ Si region. Microstructure holes 5012 can be formed inthe Ge/GeSi, and in some cases can be within the p+ region, and in somecases can extend into the Ge/GeSi partially and in some cases can extendthrough the Ge/GeSi. The microstructure holes can be periodic and insome cases can be aperiodic, and in some cases can be periodic andaperiodic. The microstructure hole lateral dimension can range from 200nm-1800 nm, and the spacing between the holes can range from 0(intersecting)-800 nm, and in some cases can be greater than 800 nm. Themicrostructure holes can be cylindrical, funnel, conical, trapezoidal orany combination thereof. The shape of the holes can be circular, oval,amoebic, square, rectangular, triangular, polygonal, to name a few.Optical signal can impinge from the top surface, and in some cases canimpinge from the bottom surface. A reverse bias is applied between theanode and cathode with bias voltages ranging from −0.5-−10 volts, and insome cases from −1-−3.3 volts, and in some cases greater than −10 voltsfor example −35 volts.

Data rate in structures such as illustrated in FIG. 50 can range fromGb/s to 25 Gb/s and in some cases 25 Gb/s-50 Gb/s, and in some casesgreater than 50 Gb/s, and in some cases less than 10 Gb/s. Wavelengthrange can range from 800 nm to 1650 nm and in some cases 950 nm-1200 nm,and in some cases 990 nm-1350 nm, and in some cases 1000 nm-1550 nm, andin some cases greater than 1550 nm.

FIGS. 51A-D show simplified partial cross-section schematic examples ofmicrostructure holes where microstructure holes can be defined asregions where the optical refractive index is lower than in thesurrounding material. For example, FIG. 51A shows microstructure holes5112 etched in Si, and the holes have an index of 1 and Si has an indexof 3.4.

FIG. 51B is similar to FIG. 51A, and the microstructure holes 5114 areburied in a dielectric such as Si dioxide for example which can have anindex of 1.5, and the Si can have an index of 3.4.

FIG. 51C shows another example of microstructure holes where the holes5116 are composed of Si material with an index of 3.4, and thesurrounding material is Ge which can have an index of 4 at certainwavelengths. In this example the microstructure holes are the Siprotrusions.

FIG. 51D shows dielectric islands formed on Si layer where thedielectrics can be Si oxide for example and Ge grown over the dielectricislands. In this example the microstructure holes 5118 are thedielectric islands which can have a refractive index ranging from1.1-1.5, and the Ge can have a refractive index of 4 at certainwavelengths, and the Si can have a refractive index of 3.4 at certainwavelengths.

In the case of etching holes in Si in structures such as illustrated inFIGS. 51A-D, the dimension of the microstructure hole can range from300-1300 nm or more where as if the microstructure holes have an indexother than 1 the dimension of the microstructure hole can be divided bythe refractive index within the hole. For example, if the holes arefilled with Si dioxide the dimension of the hole can be divided by1.2-1.5, and in some cases where the holes are Si islands, thedimensions can range from 150 nm-800 nm and in some cases more than 800nm.

The microstructure holes in FIGS. 51A-D can be periodic, or aperiodic,or periodic and aperiodic. The lateral dimension of the holes can be thesame, and in some cases can have one or more different lateraldimensions. The depth of the microstructure holes or the height ofmicrostructure islands can be the same, or can have more than one depthor height.

FIG. 52 shows a simplified partial cross-section schematic of aninterdigitated Ge on Si SOI photodiode with lateral P and N wells withmicrostructure holes between the interdigits. The BOX layer on the Sisubstrate is approximately 100-150 nm thick and in some cases can bethinner than 100 nm. The Si device layer is I or low dope and has athickness ranging from 10-50 nm, and the Ge layer grown on the Si devicelayer is I or low dope and has a thickness range from 250 to 400 nm. TheN+ and p+ wells are formed in the Ge under the interdigitated metalelectrodes M1 and M2. The N+ and p+ wells are approximately 100 nm wide,the depth of the well can range from 10 nm to 400 nm and in some casescan be partially in the Ge and/or entirely through the depth of the Gelayer; see for example Dehlinger et. al, High-Speed Germanium-on-SOILateral PIN Photodiodes, IEEE Photonics Technology Letters, Vol. 16, NO.11, November 2004 FIG. 1 where such a structure has demonstratedresponse to 36 GHz as shown in FIG. 4. According to some embodimentsmicrostructure holes 5212 are added with diameter or lateral dimensionof 400 nm and in some cases 600 nm, and spacing between the holes of 200nm in a square lattice which can further enhance the sensitivity and canhave EQE greater than a comparable interdigitated Ge on Si SOI withoutmicrostructure holes at certain wavelengths. The microstructure holes5212 can be partially etched into the Ge and in some cases through theGe, and in some cases to the BOX layer. Not shown are passivation layerssuch as Si dioxide at the edge of the mesa and/or in some cases insidethe microstructure holes. The passivation can coat the inside walls ofthe microstructure holes, and in some cases can fill the microstructureholes with Si dioxide, Si nitride, and/or other dielectrics. Reversebias can be applied between M1 (cathode) and M2 (anode) with voltagerange of 0.1 volt to 3.3 volts or more, and in some cases 0.3 volts to 1volt. In some cases a reverse bias of 10 volts or more can result inavalanche gain. The M1 and M2 electrodes can be Al, or Ti/Al or Ni/Aland in some cases be a silicide. The width of the electrode can besmaller than the well for example 180 nm or less and in some cases canbe 60 nm or less. The well width in some cases can be less than 200 nmfor example 100 nm or less, and in some cases 50 nm or less. The lateraldimension of the photo sensitive mesa can be 10×10 microns squared andin some cases can be 30×30 microns squared, and in some cases can be50×50 microns squared. In some cases the photo sensitive area can beless than 10×10 microns squared for example 5×5 or 1×1 in which casesthe electrode width can be 14 nm or narrower. Optical signal can impingeon the top surface, and in some cases can impinge on the bottom surfaceor the substrate surface.

FIG. 53A shows a simplified 30 schematic of a Ge on Si SOI lateral PINinterdigitated photodetector, according to some embodiments. Thephotodetector shown can be a photodiode, APO, SPAD. A thin layer of Gewith thickness ranging from 100-300 nm I or low dope can be grown on athin layer of Si device layer with a thickness ranging from 5 to 200 nmon a BOX layer with thickness ranging from 10 to 1000 nm on Si handlelayer/wafer. P and N wells can be formed in the Ge that can be p+ or N+doped with depth ranging from 10 nm to 100 nm, and in some cases 10nm-50 nm, and in some cases less than 20 nm. Interdigitated electrodes5320 can be formed on the P and N region forming ohmic contacts to the Pand N wells, and the metal can be Ti/Al, Cr/Al, Al, Nil Al, Ti/Cu,Cr/Cu, Cu to name a few. Microstructure holes 5312 can be etched intothe Ge and can be partially etched into the Ge, and in some casesthrough the Ge to the BOX layer, and in some cases through the Ge layerto the Si layer. The microstructure holes 5312 can have lateraldimensions ranging from 100 nm to 1000 nm or more, and in some cases 300nm-1200 nm. The spacing between the interdigitated electrodes can rangefrom 300 nm to 1000 nm and in some cases 200 nm-600 nm, and in somecases less than 200 nm, and in some cases more than 1000 nm. The widthof the electrodes 5320 and the doped wells can range from 10 nm to 300nm, and in some cases 30 nm-160 nm. The doped wells can be a littlewider than the interdigitated electrodes.

The wavelength of the optical signal in structures such as illustratedin FIGS. 53A-B can range from 800 to 2000 nm, and data rate can rangefrom 25 Gb/s to 50 Gb/s and in some cases 40 Gb/s-60 Gb/s or higher.

Very shallow P and N wells, with well depth of 5-20 nm and with N+p+ orN++ p++ and/or degenerate doping, and in some cases P and N doping canbe used in structures such as illustrated in FIGS. 53A-B to minimize thenumber of photo generated carriers in regions with low electric fields.

FIG. 53B shows a simple 30 schematic of an interdigitated lateral PINphotodetector with interdigitated electrodes such as shown in FIG. 52.See for example reference, Koester et. al,Ge-on-SOI-Detector/Si-CMOS-Amplifier Receivers for High-PerformanceOptical-Communication Applications, Journal of Lightwave Technology,Vol. 25, No. 1, January 2007, compatible with CMOS/BiCMOS process andwhere 15 Gb/s data rate was demonstrated. According to some embodimentsof this patent specification, microstructure holes 5314 are added.

FIGS. 54A-C show FDTD simulated optical absorption of a structure suchas shown in FIG. 52. In FIG. 54A the structure has cylindrical holeswith diameter of 400 and 600 nm with spacing of 200 nm in a squarelattice and with Ge thickness of 250 nm. The microstructure holes areetched through the Ge to a depth of 250 nm, Al electrode width of 180nm. The absorption which is directly proportional to EOE is shown forwavelength range from 800 to 1000 nm. The solid curve 5410 is for holesof 600 nm, and the dashed curve 5412 is for holes of 400 nm diameter.The absorption or EOE can be greater than 50% at wavelength range from800 to 1000 nm, the EOE of microstructure hole PD can be higher than acomparable PD without microstructure holes at certain wavelengths.

FIG. 54B shows FDTD simulation of a structure similar to that simulatedin FIG. 54A with wavelength range from 1000-1700 nm where themicrostructure holes are etched to ½ the depth of the Ge layer. Thesolid curve 5420 is for cylindrical holes with diameter of 600 nm, andthe dashed curve 5422 is for cylindrical holes with diameter of 400 nm,and where the holes have a 200 nm spacing in a square lattice. Theabsorption or EOE can be greater than 30% at 1350 nm, and in some casescan be greater than 10% at 1350 nm.

EOE in the example of FIG. 54B can be as high as 70% at certainwavelengths and data rate can be 40 Gb/s or higher, and in some cases40-60 Gb/s.

FIG. 54C is similar to FIG. 54B with the exception that themicrostructure holes are etched through the Ge layer to the Si layer.The solid curve 5430 is for the case of cylindrical holes with adiameter of 600 nm and the dashed curve 5432 shows cylindrical holeswith a diameter of 400 nm. Lateral interdigitated PIN Ge on Si SOI withmicrostructure holes can have an EOE higher than a comparablephotodetector without microstructure holes at certain wavelengths. TheEOE of the microstructure hole lateral PIN Ge on Si SOI can be 10% orhigher at wavelength of 1550 nm. The absorption is directly proportionalto EOE and in some cases can be equal to EOE.

FIG. 55 shows experimental data of external quantum efficiency vs.reverse bias voltage of an interdigitated MSM photodetector on SOI wherethe device layer is 1 micron thick in structures such as illustrated inFIG. 47C and in other new lateral Schottky MSM structures described inthis patent specification. The BOX layer is approximately 1 micronthick, and a handle Si substrate of approximately 700 microns thick. Thedevice layer is low dope P type with a resistivity approximately 10-25ohm-cm, and where the metal interdigits are Al forming a Schottkycontact with the low dope P Si. Microstructure holes with 1000 nmdiameter, and 1300 nm period in a square lattice. The holes are dryetched using drie (deep reactive ion etching) to a depth ofapproximately 600-800 nm. The width of the interdigit Al electrodes are300 nm wide, and the spacing is 1000 nm wide. 850 nm wavelength impingeon the top surface using multimode or single mode fiber. The trianglesin the graph shows the EQE of a controlled sample without microstructureholes, and as can be seen the EQE is approximately 13-14% which agreeswith theoretical calculations. The squares is the EQE of a MSMphotodetector with microstructure holes that is not passivated and ascan be seen the maximum EQE attained is just over 30% at −10 volts. Thecircles shows the EQE of the same MSM photodetector with microstructureholes that are passivated with Hydrogen, and as can be seen, the EQE isapproximately 85% which is close to the theoretical prediction of 86%.The theory is using FDTD simulation of the optical fields in the MSMstructure with and without holes and with the metal interdigits fingersin place at 850 nm. As can be seen, passivation in this case usingHydrogen (3 second dip in diluted HF solution) can reduce surfacerecombination at the side walls of the holes to a point where virtuallyall the absorbed photons can be collected so that EQE is approximatelyequal to number of absorbed photons. Other passivation methods caninclude thermal oxide of the Si, deposition of dielectrics such as Aloxide, Si dioxide, Si nitride, Hf oxide to name a few using methods suchas atomic layer deposition. The passivating oxides can be formed on thesurface of the substrate and the surface of the side walls of themicrostructure holes, and in some cases can partially and/or entirelyfill the microstructure holes. This experimental data of EQE for a 1micron device layer SOI shows good agreement with FDTD simulations forMSM structures.

FIGS. 56A-D show the impulse responses at 850 nm wavelength of a devicewith EQE shown in FIG. 55. As can be seen, FIGS. 56A and 56C are for MSMwith microstructure holes at 3 and 10 volt bias respectively, and FIGS.56B and 560 are controlled samples on the same wafer withoutmicrostructure holes. As can be seen, the amplitude of the impulseresponse of the MSM without microstructure holes is significantly lowerthan for an MSM with microstructure holes and passivated with Hydrogen.The full width half max is 38 picoseconds and if the system timeconstants such as the laser pulse width and the response time of thesampling scope are deconvolved the full width half max can besignificantly shorter than the 38 pico seconds measured for the MSMphotodetector with 50 microns diameter. As can be seen, the rise timefor the impulse response is approximately 10-20 picoseconds at the10-90% amplitude level which can have a depth resolution in themillimeter range for time of flight applications such as LiDAR. For datacenter communications, data rates of 10-25 Gb/s can be obtained, andwith thinner device layer of for example 0.5 microns and with spacingbetween the electrodes of approximately 400-600 nm and with electrodewidth ranging from 160 nm-60 nm and in some cases less than 60 nm, forexample 30-14 nm, the data rate of the MSM photodetector can be greaterthan 25 Gb/s and in some cases 40-50 Gb/s, and in some cases 60 Gb/s ormore.

FIGS. 57-59 shows simplified partial cross-section of a bottomilluminated CMOS/BiCMOS sensor array, according to some embodiments.Microstructure holes 5712 enhance the absorption, and extend theoperating wavelength of the sensor array which can be used for highspeed optical data communication, time of flight applications such asLiDAR and imaging at near infrared wavelengths. CMOS/BiCMOS ASICs arefabricated in the device layer of a SOI wafer and where the handle wafercan be low dope P or N such as v or re doping for example. Thephotodetectors are fabricated in the handle substrate of the SOI andwhere microstructure holes are etched into the handle substrate towithin a few microns or less to the BOX layer. In FIG. 57, ionimplantation can be used to form N wells and P wells on a re type handlewafer. Connecting electrodes 5740 from the CMOS ASICs can be formed tothe N well through a via and the connecting electrode can be metallic,and in some cases can be metal silicide. Connecting electrodes 5740 canalso be formed from the CMOS to the P layer through a via, and in somecases the P layer can have a metallization such as an anode and can beconnected to a common ground instead of through TSV (trans silicon via).The N wells are cathodes, and the P wells are anodes, and a reverse baiscan be applied between the anode and cathode. The handle wafer thicknesscan range from 200 microns to a few microns for example 3 microns. Themicrostructure holes 5712 can be etched in the handle substrate towithin a few microns of the BOX layer, in some cases to within 3 mirconsor less or the BOX layer, and in some cases to within 1 micron or lessto the BOX layer. The microstructure holes can have a diameter rangingfrom 300 nm-1500 nm, and in some cases from 500 nm-1500 nm, and in somecases from 700 nm-1800 nm, and in some cases 800 nm-1200 nm. The spacingbetween the microstructure holes can range from 100 nm-600 nm, and insome cases more than 600 nm. The microstructure holes can be periodic,and/or aperiodic, and/or random. The microstructure hole diameter orlateral dimension can be the same and/or in some cases can vary withinthe same array. The microstructure holes can be circular, oval, square,rectangular, polygonal, and/or amoebic. The microstructure holes can bedry etched using ORIE for example and in some cases can be a combinationof dry and wet etch using TMAH for example. The surface of themicrostructure holes and of the Si can be passivated with native oxideand in some cases with dielectrics that can be deposited on the surfaceusing atomic layer deposition for example to reduce surfacerecombination and thereby to increase the EOE. The passivationdielectrics can partially fill the microstructure holes, and in somecases fill the microstructure holes entirely. The N wells can be ionimplanted and then activated with thermal anneal, and the P wells canalso be ion implanted and activated with thermal anneal. In some casesthe P and N wells can be formed by diffusion and/or a combination of ionimplant and diffusion of dopant ions. By etching the microstructureholes, the N wells can be formed close to the BOX layer irrespective ofthe thickness of the TT Si, for example in some cases the TT Si can be50 microns or thicker and with microstructure holes etched to within afew microns of the BOX layer the N wells can be ion implanted in closeproximity to the BOX layer, and in some cases touching the BOX layer.Electrodes can be formed from the CMOS/BiCMOS ASICs to the N wellcathode region, and anode can be formed on the P well and can beconnected to the CMOS/BiCMOS ASICs. Optical signal which can be highdata rate signal, time of flight optical pulses, or images canilluminate the back surface with wavelength range of 800-1100 nm, and insome cases 900-1060 nm, and in some cases 1000-1100 nm wavelength. Withhandle layer thickness of 10 microns or less data rates can be greaterthan 1 Gb/s. With handle layer thickness of 3 microns or less, datarates can be 10 Gb/s or more. EQE of microstructure hole backilluminated CMOS sensor array can be greater than a comparable backilluminated CMOS sensor array without microstructure holes at certainwavelengths. See reference Lee et. al, A Back-Illuminated Time-of-FlightImage Sensor with SOI-Based Fully Depleted Detector Technology for LiDARApplication, Proceedings 2018, 2, 798; doi:10.3390/proceedings2130798.Also see for example, Yokogawa et. al, IR sensitivity enhancement ofCMOS Image Sensor with diffractive light trapping pixels, ScientificReports 7:3832 D01:10.1038/s41598-017-04200-y.

The isolation trenches 5760 for electrical and/or optical can be etchedto the BOX layer, and in some cases the isolation trench can bepartially etched into the handle layer and in some cases can beoptional.

FIG. 58 is similar to FIG. 57 with the exception that the N wells canalso be on the side wall of the microstructure holes 5712. In thisstructure the transit time of the photo generated carrier can be reduceddue to the proximity of the P and N well as compared to the structureshown in FIG. 57 for example. The reduction in transit time can resultin a faster photodetector. The sensor array can have array sizes rangingfrom 2×2 to 1000×1000 or more.

With N doping on the side wall of the microstructure holes in structuressuch as illustrated in FIG. 58, the handle layer of the SOI wafer can bethicker for example greater than 50 microns without significant loss inspeed due to presence of applied electric field in the absorptionregions. It should be noted that the P and N can be interchanged and thehandle substrate can be low dope P or N with resistivity greater than100 ohm-cm, and in some cases 1000 ohm-cm.

FIG. 59 shows a structure similar to FIG. 57 with the exception that Geand/or GeSi alloy can be grown on the surface of the microstructure hole5712. P and N wells are formed in contact to the Ge/GeSi layer. With theaddition of Ge/GeSi the wavelength of back illuminated CMOS/BiCMOSsensor array can be extended to 1800 nm, and in some cases from 1000nm-1600 nm. The EQE of a microstructure hole back illuminated arraysensor can be greater than a comparable back illuminated sensor withoutmicrostructure holes at certain wavelengths.

The Ge/GeSi on Si structures illustrated in FIG. 59 can form aPD/APO/SPAD array.

FIGS. 60A and 60B show a cross-section view and bottom view,respectively, of a microstructure hole back illuminated CMOS/BiCMOSsensor array, according to some embodiments. The microstructure holes6012 are etched to within a few microns of the BOX layer for exampleless than 2 microns. The P and N dopant ions are diffused into the sidewall of the microstructure holes, and adjacent microstructure holes canhave a different dopant polarity as shown in FIG. 60. The PIN structureare lateral and provide strong electric fields within the absorptionregion, and where the handle wafer can have thicknesses ranging from200-1 micron thickness. Reverse bias can be applied to the doped regionof anode and cathode via connecting electrodes that can be metallic ormetal silicide through the BOX layer to the CMOS/BiCMOS ASICs.

The microstructure holes 6012 can have a lateral dimension ranging from400-1800 nm and in some cases 600-1200 nm and can be circular, oval,square, rectangular, polygonal, hexagonal, and/or amoebic and can havean etch depth ranging from 10 microns to 200 microns, and in some casesless than 10 microns. In some cases, the etch depth can range from 1micron to 50 microns. The microstructure holes are dry etched using ORIEfor example and can be a combination of dry and wet etch where the depthof the etch is not limited by facet angles such as in the case ofinverted pyramids where the depth is limited by crystal planes of 54degrees approximately. The microstructure holes can be periodic and/oraperiodic, and/or random. The holes can be passivated with a dielectricand can partially or fully fill the microstructure holes.

The lateral PIN of FIGS. 60A-B can be a photodiode and, in some cases,APO and in some cases SPAD arrays and in some cases can be a combinationof PD, APO, SPAD in an array. A reverse bias can be applied between theN cathode and the P anode with reverse bias voltages ranging from 0.5volt −3.3 volts, and in some cases 1 volt-10 volts, and in some casesfrom 1 volt-35 volts, and in some cases greater than 35 volts. The speedor data rate bandwidth or the 10-90% rise time can be determined by thephoto generated carriers in the Si/GeSi/Ge transit time and capacitance.The CMOS/BiCMOS ASICs for data center interconnect applications canconsist of trans-impedance amplifiers and other electronics needed forsignal processing and communication of the processed electrical signalwith other components in the data center, and in some cases the ASICscan also include electronics for biasing and controlling APO/SPADdevices and all the necessary electronics for conditioning, processingand transmission of the electrical signal, and in some cases the ASICscan also include electronics for image processing such as 3D imageprocessing, and read out electronics, and necessary electronics fordisplaying an image, and in some cases the ASICs can also include timeof flight electronics and necessary processing electronics to determinespatial and depth resolutions such as for LiDAR applications. Opticalsignal and/or optical image impinge on the bottom surface.

Ge and/or GeSi can also be grown within the holes as in FIGS. 59 and 60Ato form a lateral Ge on Si PIN PD/APO/SPAD.

The data rate in structures such as illustrated in FIGS. 60A-B can rangefrom 10 to 50 Gb/s or more, and in some cases 25-50 Gb/s or more, andthe 10-90% rise time can range from 5 ps to 100 ps, and in some cases 10ps-100 ps. The gain can range from 3 dB to 30 dB or more, and thewavelength range without Ge or GeSi can range from 500 to 1100 nm, andwith Ge/GeSi can range from 500 to 2000 nm, and in some cases t800-2000nm.

In SPAD mode the gain in structures such as illustrated in FIGS. 60A-Bcan range from 100,000-1,000,000 or more.

With doping profiles of PN, PIN, PIPN in structures such as illustratedin FIGS. 60A-B, the photodetector can be a photodiode or an avalanchephotodiode, or a single photon avalanche photodiode. The spacing betweenthe microstructure holes can range from 100 nm-500 nm. The thickness ofthe photodetector layer can range from 30 nm to-5000 nm, and in somecases 300 nm-3000 nm. The photodetector can be back illuminated CMOSimage sensor or a front illuminated CMOS image sensor. A reverse bias isapplied between the anode (P) and cathode (N) with a reverse biasvoltage ranging from 0.7 V to 35 V and in some cases 0.7 V-3.3 V, and insome cases 3.3 V-15 V.

FIG. 60B is single pixel bottom view where the microstructure holes 6012have lateral P and N doped regions, and the holes are arranged such thatthe neighboring holes have opposite doping polarities. An isolationtrench can be included where the isolation trench can be partiallyetched into the bottom handle layer, and in some cases it can be fullyetched to the BOX layer.

The microstructure holes 6012 can be circular, oval, polygonal, amoebic,and can be in a periodic or aperiodic or random arrangement. Themicrostructure holes can be cylindrical, funnel or conical shaped. Thelateral dimension of the hole can range from 300 to 1500 nm and in somecases more than 1500 nm. In some cases, the lateral dimension of theholes can range from 500 to 1200 nm. The spacing between the holes canrange from 100 nm to 600 nm, and in some cases from 300 nm to 1000 nm,and in some cases more than 1000 nm.

FIGS. 61 and 62 are simplified partial cross-sections of amicrostructure hole bottom illuminated CMOS/BiCMOS sensor array,according to some embodiments. In FIG. 61, the microstructure hole 6112can be etched to the BOX layer and N dopant ions are diffused into thesidewalls. P wells can be formed on the bottom surface. Connectingelectrodes can be formed through the BOX layer from the CMOS/BiCMOSASICs, and connect to the N doped layer to form a cathode. Anodemetallization can be formed on the P layer and can be connected to theCMOS/BiCMOS ASICs through a common ground and/or through a TSV. Only onemicrostructure hole is shown however, multiple holes forming a periodicand/or aperiodic and/or random array can be formed.

FIG. 62 is similar to FIG. 61 except that multiple holes 6212 are shownand connected via a common electrode to the CMOS/BiCMOS ASICs. Thenumber of holes connected can range from 1 to 1000 or more, and in somecases 1-100, and in some cases can be more than 1000 holes, for example10,000-1000,000 holes or more.

FIGS. 63A-B show a simplified partial bottom schematic views of a backilluminated CMOS/BiCMOS sensor array with circular holes. In FIG. 63A,periodic circular holes 6312 are arranged in a square lattice. FIG. 63Bshows an aperiodic and/or random arrangement of microstructure holes6312. Each pixel of the sensor array depending on the size of the pixelcan contain anywhere from a single to 1000 microstructure holes or more,and in some cases from 5-30 microstructure holes, and in some cases 100or more microstructure holes. In some cases, the number of holes canrange from 1000 to 10,000 within a pixel or photosensitive area. Thespacing between the microstructure holes can range from 100 nm to 600nm, and in some cases more than 600 nm for example 1,000 nm.

FIG. 64 is a diagram illustrating hexagonal holes in a hexagonallattice, according to some embodiments. The holes 6412 can be fabricatedusing dry etching and the depth of the holes can be etched to the BOXlayer, and in some cases to within 1 or 2 microns of the BOX layer. Thespacing between the hexagonal holes can range from 100-500 nm, and insome cases 300-600 nm. The lateral dimension of the hexagonal holes canrange from 300 to 1800 nm, and in some cases 600-1200 nm, and in somecases 800-1000 nm.

An isolation trench 6460 can be etched into the bottom surface partiallyinto the handle layer, and in some cases through the handle layer to theBOX layer. The isolation trench can be for electrical isolation betweenpixels and/or optical isolation between pixels. Shown in FIG. 64 can bea single pixel or multiple pixels in an array that can have 1-1,000,000or more pixels and applications can include optical data communication,LiDAR and 3D imaging, and in some cases time of flight imaging.

FIG. 65 shows a FDTD simulated optical absorption vs wavelength for a 1micron device layer on SOI with microstructure holes diameter of 1000 nmand 1300 nm period in a square lattice in structures such as illustratedin FIG. 47C and in other new lateral Schottky MSM structures describedin this patent specification. The dashed curve 6510 shows absorption ofthe 1 micron Si layer on a BOX layer with microstructure holes withabsorption greater than 30% from 800 to 1100 nm at certain wavelengths.The solid curve 6512 shows the absorption of a 1 micron Si layer withoutmicrostructure holes. As can be seen, the absorption by the layer withmicrostructure holes can be 20-30% or more greater than that of theabsorption of a 1 micron layer without microstructure holes at certainwavelengths.

FIG. 66 shows a FDTD simulation of a 0.5 micron Si device layer on SOIin structures such as illustrated in FIG. 47C and in other new lateralor vertical Schottky MSM structures described in this patentspecification. The microstructure holes for the solid curve 6610 is 1000nm diameter and 1300 nm period in a square lattice, and the dashed curve6612 is for microstructure hole with 600 nm diameter and 900 nm periodin a square lattice. As can be seen, the absorption to which the EOE isdirectly proportional to can be 10% or greater at 1100 nm wavelength.

FIGS. 67A-B are linear and semi-log plots, respectively, of the IVcharacteristics with and without 850 nm wavelength illumination instructures such as illustrated in FIG. 47C and in other new lateralSchottky MSM structures described in this patent specification.

Illumination curve 6710 seen as in FIG. 67A is characteristic of back toback Schottky contacts of aluminum interdigitated electrodes to the Sidevice layer which have a resistivity ranging from 10 to 25 ohm-cm. Thespacing between the interdigitated fingers is 1000 nm and the width ofthe interdigitated fingers is 300 nm and the lateral diameter of thephotosensitive area of the interdigitated photodiode is 50 microns.

FIGS. 68A-D and 69A-D show impulse responses and eye diagrams of aninterdigitated Si MSM with microstructure holes in structures such asillustrated in FIG. 47C and in other new lateral Schottky MSM structuresdescribed in this patent specification, according to some embodiments.The microstructure holes have diameter of 1000 nm and a period of 1300nm in a square lattice with a 1 micron device layer on a SOI substrate.FIGS. 68A and 68C are two impulse responses for two different devices onthe same wafer at 10 volts reverse bias. The consistency of theperformance of the devices can be seen. The respective eye diagrams ofFIGS. 68B and 68D at 10 Gb/s with a volt reverse bias.

FIG. 69A-D are impulse responses and eye diagrams from the same devicesas in FIG. 68A—but with a 3 volt reverse bias. The 10 Gb/s eye diagramshown below the impulse response where the eyes are open and can be usedfor 10 Gb/s data rate transmission in a DCI application.

FIG. 70 shows the percentage of the capacitance change of a PIN/NIPvertical structure photodetector with and without microstructure holesin vertical PIN structures such as illustrated in FIG. 14A. As can beseen in the experimental data the capacitance can be 50% or more lessfor a photodetector with microstructure holes as compared with acomparable photodetector without microstructure holes. This reduction incapacitance can result in a reduced RC time constant which can translateto higher speed or data rate bandwidth for a photodetector which can bea PD, APO, or SPAD than a comparable PD/APO/SPAD without microstructureholes.

FIG. 71 shows FDTD simulated optical absorption in Si layers on SOI. TheSi device layer range from 1000 nm-200 nm as shown in the plots.Microstructure holes have lateral dimension of 700 nm and period of 1000nm in a square lattice. The microstructure holes are cylindrical and areetched to the BOX layer. The vertical axis is absorption, and thehorizontal axis is wavelength from 800-1100 nm. The absorption isproportional to EQE and in some cases can be approximately equal to EQE.The absorption can be 50% or greater at a wavelength of 1050 nm forthicknesses of 500 nm Si device layer, and can be 20% or greater forthicknesses of 200 to 300 nm device layer. With electrode spacing of 300nm to 500 nm and with device layer of less than 500 nm data rates can be30 Gb/s or higher and in some cases 25-50 Gb/s, and in some cases morethan 50 Gb/s, and in some cases 100 Gb/s or greater.

FIGS. 72A-B show simplified partial cross-sections of a Si MSM,according to some embodiments. The Si MSM can be monolithicallyintegrated with CMOS/BiCMOS ASICs. The device layer of the SOI can bevery thin with thickness ranging from 50 to 500 nm, and in some cases300-1000 nm. The interdigitated electrodes 7220 and 7222 can have widthranging from 20 to 160 nm, and in some cases 30-60 nm, and the spacingbetween the interdigitated electrodes can range from 100 to 600 nm. Withsuch spacing and thickness the MSM can have data rates of 30 Gb/s ormore, and in some cases 25-50 Gb/s, and in some cases 30-60 Gb/s, and insome cases 60-100 Gb/s or more. EQE can be 20% or greater at certainwavelengths, and in some cases 50% or greater at certain wavelengths,and in some cases 70% or greater at certain wavelengths, where thewavelength range can be from 800 to 1100 nm. The metal electrodes canform Schottky contacts to the I or low dope Si, and in some cases PNjunctions that can be medium or high doped wells 7210 and 7208 can beformed under the electrodes and where the electrodes form ohmic contactsto the P and N junctions. The depth of the P and N junctions can rangefrom 10 nm to 500 nm, and in some cases more than 500 nm. Shallow PNjunctions with depth ranging from 5 to 30 nm may be desirable tominimize the number of photo generated carriers in regions with lowelectric fields. The width of the P and N wells 7210 and 7208 can be thesame or slightly wider than the width of the interdigitated electrodes.A reverse bias is applied between the P anode and N cathode. In the caseof Schottky contacts the MSM can be operated both in the reverse andforward bias since the IV can be approximately symmetric.

Microstructure holes 7212 are etched partially into the Si device layer,and in some cases through the Si device layer to the BOX layer. Themicrostructure holes 7212 can be fitted with Si dioxide and/or otherdielectrics. The microstructure holes 7212 can be rectangular or ovalwhere the narrow lateral dimension can range from 100 to 600 nm and theY lateral dimension can range from 300 nm-1000 nm or more and in somecases from 600 nm to 1700 nm.

FIG. 728 is similar to FIG. 72A except with the addition of Ge/GeSi onSi that can be globally grown and/or selective area grown. The Ge layercan have a thickness ranging from 100 to 500 nm and the Si can have athickness ranging from 10 to 300 nm or more. The BOX layer can beoptional. The thickness of the BOX layer can range from 10 to 1000 ormore on a Si handle layer or substrate. The Ge and the Si can be I orlow doped. Wells of P and N can be formed in the Ge under the M1 and M2electrodes. Wavelength can range from 800 to 2000 nm, and data rates canrange from 25 to 50 Gb/s, and in some cases 40-60 Gb/s, and in somecases 60-100 Gb/s or more. A reverse bias is applied between the Panode, and the N cathode with voltages ranging from −1 volt to −3.3volts, and in some cases for APO/SPAD the reverse bias voltage can rangefrom −3.3 volts to-volts or more. The EQE can be 20% or more at certainwavelengths, and in some cases can be 50% or more at certainwavelengths, and in some cases can be 70% or more at certainwavelengths. Optical signal can impinge from the top and/or from thebottom surface.

Not shown in FIGS. 72A-B are CMOS/BiCMOS ASICs that can bemonolithically integrated.

Applications for these lateral PIN interdigitated photodetectorsdescribed above can include data center interconnect, time-of-flightLiDAR, LiDAR imaging, and/or 3D imaging to name a few. Such detectorscan be fabricated in arrays to increase the aggregated data ratebandwidth for data center applications and in some cases high densityarrays for example 10,000-1,000,000 pixels for high resolution LiDARimaging and/or 3D imaging.

The lateral dimension of the microstructure hole can be divided by theoptical refractive index of the material that fills the microstructurehole in some cases.

FIG. 73 shows a simplified partial schematic of a top view of the devicedepicted in FIGS. 72A-B. The microstructure holes 7212 can havedifferent lateral dimensions such as long and narrow. Such holes 7212can be polarization sensitive and can be used for polarization opticalmultiplexing where selective polarization of light can increase the databandwidth of an optical system in the case where polarizationsensitivity of photodetectors is not desirable. The elongatedmicrostructure holes can be formed in orthogonal orientations withcorresponding interdigitated electrodes as discussed above.

With the interdigitated electrodes 7220 and 7222 crossing themicrostructure holes as shown in FIG. 73 photo generated carriers in theSi or Ge/GeSi have a clear path to the electrodes and are not impeded bythe microstructure holes which can result in a faster MSM photodetector.In such arrangements the spacing of the electrodes are not limited bythe size of the microstructure holes.

FIG. 74A-B shows cross-section schematics of Ge and/or GeSi selectivearea grown on regions where there is Si. In FIG. 74A, starting with aSOI wafer a front end of line process (FEOL) where Ge and/or GeSiphotodetector can be fabricated prior to the CMOS/BiCMOS electronics orASICs. A pattern of microstructure holes 7412 can be etched in thedevice layer to the BOX layer and where the BOX layer can be optional insome cases. In the case where the BOX layer is optional, a dielectriclayer can be deposited on the Si surface where the holes are etched suchas at the bottom of the holes. Ge and/or GeSi can then be grown on theSi surface to form a pattern of Ge/GeSi layer with microstructure holes.In this case the holes formed in Ge and/or GeSi are by selective areagrowth and not by etching such as dry etching or wet etching. Theadvantage of forming the microstructure holes by epitaxial growth isthat the surface of the holes are not damaged by etching and can lead toreduced dark current, and/or recombination of photogenerated carriers. Pwells 7410 and N wells 7408 can be formed in the Ge and/or GeSi asshown, and ohmic electrodes can be formed on the surface of the P and Nwells. A reverse bias can be applied to the anode (P), and cathode (N)with reverse bias voltage ranging from −1 to −10 volts and in some casesgreater than −10 volts. The electrodes can form the interdigit fingersM1 and M2 of an interdigitated lateral photodiode.

FIG. 74B is similar to FIG. 74A except that the holes are filled with adielectric 7430, and the surface can be planarized using chemicalmechanical polishing (CMP). Electrodes can be formed over the dielectricfor example. An example of electrodes crossing the dielectric is shownin FIG. 73 where the electrode for example M2 crosses both the dialecticand the Ge and/or GeSi as shown in FIGS. 72A-B which can be a top viewof FIG. 74B.

The lateral dimension of the microstructure holes can be divided by theoptical refractive index of the material that fills the microstructurehole in some cases.

FIG. 75A shows a top view of the device shown in FIG. 74A. Not shown inFIG. 75A is the transmission line connecting transmission line M1 andtransmission line M2 to the CMOS/BiCMOS ASICs. In addition, a singlephotodetector is shown and multiple photodetectors such as photodetectorarray 1×4, 2×4 or higher order arrays can be integrated on a single chipand connected to corresponding CMOS/BiCMOS ASICs electronics for furthersignal processing.

FIG. 75B shows a simplified top view of FIG. 74B, and not included arethe transmission lines connecting the photodiode to the CMOS/BiCMOSASICs, and in this case multiple detectors and be formed on a singlechip and connected to the corresponding electronics for further signalprocessing.

Monolithic integrated photodetectors to corresponding CMOS/BiCMOS ASICshave significant reduction in parasitic capacitance and inductance thatcan significantly improve performance and yield. In prior art caseswhere the photodetector or photodetector arrays are wire bonded tocorresponding CMOS/BiCMOS ASIC chips, and/or other electronic chips theparasitic inductance of the wire-bond can significantly degrade theyield such that active optical and electric testing may be required foreach unit prior to shipping which can greatly increase the cost of areceiver optical sub assembly (ROSA). In the case of monolithicintegrated photodetector/photodetector arrays with CMOS/BiCMOS ASICswith significant reduction in parasitic capacitance, resistance, andinductance as described in this patent specification the performance issignificantly better in terms of bandwidth and sensitivity than in awire bonded prior art device. In addition the monolithic integratedphotodetector array and CMOS/BiCMOS ASICs described in this patentspecification benefit from manufacturing uniformity and significantlyhigher yield such that only spot testing is required, and can thereforesignificantly reduce the cost of a ROSA

FIG. 76 shows a simplified top view of a device such as shown in FIG.74A where two interdigitated electrodes are formed on the Ge and/or GeSisurface in close proximity to the holes 7612. In this configurationphotocarriers generated in the Ge and/or GeSi can be quickly swept tothe M1 and M2 electrodes formed as shown, and the photo-generatedcarriers do not have to go “around” a hole. This arrangement ofelectrodes can be on any interdigitated photodetector formed on Siand/or Ge and/or GeSi surfaces with microstructure holes that can befilled fully or partially with a dielectric according to embodimentsdescribed in this patent specification.

FIGS. 77A-B shows a simplified partial cross-section and top viewrespectively of Si dioxide/dielectric deposited on a Si surface andwhere holes configured as slots 7702 form a pattern such as across-hatch. The slots can be formed by etching to form Sidioxide/dielectric islands.

FIG. 77B shows an example where the Si dioxide/dielectric covers overareas with growth of Ge and/or GeSi are not desired. The exposed surfaceof Si as shown are areas where Ge/GeSi can be grown with or without alow temperature buffer of Ge and/or GeSi.

FIG. 78A shows a simplified partial cross-section schematic of selectivearea epitaxial growth of Ge and/or GeSi on Si and where the surface canbe planarized using CNP for example. The thickness of the Ge and/or GeSi7810 can range from 100 to 400 nm and in some cases 200-600 nm, and insome cases 50-450 nm. The Ge and/or GeSi 7810 can be I or low doped N orP.

FIG. 78B shows a simple partial top view schematic of FIG. 78A showingareas where Ge and/or GeSi are selective area epitaxially grown in across-hatch pattern.

The lateral dimension of the microstructure hole can be divided by theoptical refractive index of the material that fills the microstructurehole in some cases.

FIG. 79A shows a simplified partial schematic of the cross-section ofFIG. 788 where p+ and N+ wells are formed on the Ge/GeSi and can be atthe same time p+ and N+ wells formed for the PMOS and NMOS for example.

FIG. 798 shows a simplified partial cross-section schematic where ohmicelectrodes are formed on the P and N wells and can be the M1 and M2electrodes forming the interdigitated Ge and/or GeSi photodiode.Connecting electrodes 7924 are also shown formed between the PMOS andNMOS and the p+ and N+ wells below them.

FIG. 80 shows a simplified partial schematic top view of FIG. 798. Theinterdigitated electrodes 8020 and 8022 are connected to transmissionlines that are connected to CMOS/BiCMOS ASICs electronics for furthersignal processing. Optical signal impinges on the top surface and insome cases can impinge from the bottom surface. The microstructure holes8012 in Ge and/or GeSi layer formed by Si dioxide and/or dielectricislands can have a diameter or lateral dimension ranging from 400 nm to1500 nm and in some cases from 400 nm-1200 nm. The shape of themicrostructure holes 8012 can be square, rectangular, oval and circular.And in addition, the microstructure holes can be periodic and/oraperiodic. The spacing between the microstructure holes can range from100 nm to 500 nm and in some cases 300 nm-1000 nm. The photodetector canbe singular and/or multiple such as in a array and are connected toCMOS/8iCMOS electronics. The lateral dimension of the photodetector canrange from 1 micron to 1000 microns or more. For optical datacommunication the lateral dimension of the photodetector can range from5 microns-50 microns and in some cases from 50 microns-1000 microns ormore. For LiDAR applications the lateral dimension can range from 10microns-1000 microns, and in some cases more than 1000 microns. Forimaging applications the lateral dimension can range from 1 micron to100 microns, and in some cases greater than 100 microns. The wavelengthcan range from 800 nm to 1650 nm and in some cases 800 nm-1350 nm, andin some cases 1000 nm-1400 nm, and in some cases 1100 nm-1550 nm.Photodetectors with microstructure holes can have higher externalquantum efficiency than an equivalent photodetector withoutmicrostructure holes at certain wavelengths. Data rate can range from 1Gb/s to 100 Gb/s or more for data center interconnect applications. Andfor time-of-flight applications the 10-90% rise time can range from 1picosecond to 100 picoseconds. For imaging the EOE of an imaging sensorwith microstructure holes can be higher than the EQE of a similarimaging sensor without microstructure holes at certain wavelengths. Areverse bias is applied between the anode and cathode.

FIGS. 81A-D show simplified partial schematic cross-sections of aninterdigitated Si photodiode on SOI wafer. In FIG. 81A, themicrostructure holes 8112 are etched to the BOX layer, and in some casesinto the BOX layer. P and N wells can be formed at the same time as theP and N wells for the PMOS and NMOS transistors. Ohmic electrodes can beformed on the p+ and N+ wells and can be the interdigitated fingers of alateral Si photodiode with microstructure holes. In some cases, themicrostructure holes can be filled with a dielectric and the surface canbe planarized using CMP for example. The devices layer can haveresistivity ranging from 10 to 1000 ohm-cm or more, and the thickness ofthe Si device layer can range from 40 nm to 2000 nm, and in some cases100 nm-2000 nm. The microstructure holes lateral dimension can rangefrom 400 nm-1200 nm, and the spacing between the microstructure holescan range from 100 nm to 600 nm, and in some cases more than 600 nm. Themicrostructure holes can be arranged in a periodic array and/or can bearranged periodically, and in some cases can be random.

FIG. 81B is similar to FIG. 81A except a trench 8124 is etched in the Sito a depth ranging from 100 to 1000 nm and where N wells 8108 and Pwells 8110 can be formed into the side walls and bottom of the trench8124 as shown. An ohmic contact electrode can be formed in the trenchwhich can be the M1 and M2 interdigits of a lateral PIN photodiode withmicrostructure holes.

FIGS. 81C and 81D are similar to FIGS. 81A and 81B respectively. In thecase of FIG. 81C a deep p+ region 8130 is formed close to the Si BOXinterface. The p+ region 8130 extends over the entire region of thephoto sensitive area and can be formed by deep ion implantation of boronions for example. An anode electrode 8126 is formed from the surface tothe deep p+ region. A reverse bias is applied between the anode whichincludes the anode M1 and the cathode M2. The electric field between thedeep p+ anode 8126 and the shallow cathode can assist in sweeping outthe photo-generated carriers to the anode and cathode under a reversebias.

FIG. 81D is similar to FIG. 81B with the exception of a deep N+ region8132 extending over the entire bottom surface of photo-sensitive regionwhich can be formed by ion implantation of phosphorous, and/or nitrogenions for example. A deep electrode contact 8128 is made to the N+ regionforming the cathode. A reverse bias is applied between the M1 anode, andthe M2 cathode, and the deep cathode. P and N can be interchanged.

FIG. 82A shows a simple partial cross-section of a Si lateral PINphotodetector with microstructure holes formed on an SOI wafer. Themicrostructure holes 8212 are etched into the device layer partially orfully. As shown the microstructure holes are etched to the BOX layer.The Si device layer can have a thickness ranging from 120 nm to 2000 nmand in some cases from 1000 nm to 2000 nm, and in some cases 200 nm-1000nm. The Si device layer can be I or low dope P or N and have resistivityranging from 10 to 1000 ohm-cm or more. P and N wells are formed intothe side walls of the microstructure holes and in some cases wherepartially etched holes in the device layer the P and N wells can beformed in the side walls of the holes and at the bottom of the holes.The microstructure holes 8212 can be circular, oval, rectangular,square, polygonal for example. The lateral dimension of themicrostructure hole can range from 400 nm to 1200 nm, and in some cases600 nm-1000 nm, and in some cases greater than 1200 nm. The spacing ofthe holes can range from 100 nm to 500 nm, and in some cases from 300nm-1000 nm, and in some cases 600 nm-1500 nm, and in some cases greaterthan 1500 nm.

FIG. 82B shows a top view schematic of FIG. 82A where the microstructureholes 8212 are arranged in a hexagonal pattern. Connecting electrodes8220 are formed connecting the P holes to the P transmission line 8240,and connecting electrodes 8222 are formed to connect the N holes to theN transmission line 8242. The connecting electrodes can also form anohmic contact to the p+ and N+ regions. In some cases additionalelectrodes can be formed on the Wand p+ region and connect to theconnecting electrodes. And in some cases transparent metal conductingoxide can be formed on the p+ and N+ region to reduce series resistance.Photo-generated carriers in the Si between the microstructure holes caneasily be swept to the anode or cathode and the bandwidth of the deviceis not determined by the thickness of the device layer, but rather bythe distance between the p+ and N+ microstructure holes which can beengineered with a distance ranging from 100 nm to 1000 nm, and in somecases 200 nm-600 nm. The transmission line connects to CMOS and BiCMOSASICs, not shown are isolation trenching optically and/or electricallythat may be needed for optimum performance of the photodetector and theelectronics. A single photodetector is shown however multiplephotodetectors such as an array can be formed connecting to appropriateCMOS/BiCMOS ASICs for further signal processing and transmission toother electronic components. In addition the entire monolithicintegrated chip can be hermetically sealed using a dielectric and/orpolymer and eclectic contacts can be formed solder bump technology andtrans silicon vias at the bottom of the chip, and in some cases thesolder bump can be on the surface of the chip. The lateral dimension ofthe photodetector can range from 1 micron to 1000 microns or more. Themicrostructure holes can be arranged in a periodic pattern or can bearranged aperiodically. This structure in a slight variation can beformed on the back surface of a SOI wafer as discussed earlier.

FIG. 82C is similar to FIG. 82B except the microstructure holes 8212 arearranged in a square pattern and where each microstructure hole with acertain polarity can be surrounded by a microstructure hole of theopposite polarity, and where the connecting electrodes can criss-crosseach other separated by a dielectric.

FIGS. 83A-C and 84A-C show FDTD simulations of optical absorption ofmicrostructure holes on SOI wafer, according to some embodiments.

FIG. 83A shows a simplified partial cross-section schematic of themicrostructure holes in Si device layer with thickness ranging from100-120 nm and the microstructure holes have dimensions of 600 nmdiameter, and period of 800 and 900 nm in a square lattice and where theholes are etched to the BOX layer. The BOX layer is 200 nm on Sisubstrate. The optical field is normal incident.

FIG. 83B shows the optical absorption vs wavelength for wavelengthranging from 800-950 nm. The various curves show the absorption vswavelength for microstructure holes with 600 nm diameter, 800 and 900 nmperiods, and Si device layer of 100 and 120 nm. In addition, a Si devicelayer of 100 nm without holes is also shown (curve 8310). Curve 8312 isfor 800 nm period and 100 nm device layer. Curve 8314 is for 900 nmperiod and 100 nm device layer. Curve 8316 is for 800 nm period and 120nm device layer. Curve 8318 is for 900 nm period and 120 nm devicelayer. As can be seen device layer with microstructure holes can have ahigh absorption than a comparable structure without microstructure holesas certain wavelengths. The external quantum efficiency is directlyproportional to the absorption and in some cases can be approximatelyequal to the absorption.

FIG. 83C shows the absorption vs wavelength for the case of a devicelayer of 70 nm thickness with holes of 600 nm diameter and 800 nm periodfor normal incident (curve 8322) and for incidents average over +/−10°(curve 8320).

FIGS. 84A-C are similar to FIGS. 83A-C with the exception that themicrostructure holes are filled with SiO2 as shown in FIG. 84A.

FIG. 848 shows the FDTD of the optical field absorption vs wavelengthfor a structure shown in figure shown in FIG. 84A. The microstructureholes are 600 nm in diameter, 800 nm period in a square lattice, andwhere the holes extend to the BOX layer. In addition the holes arefilled with SiO2. The incident optical field is normal to the surfaceand averaged by +/−10° of its normal incidence. FIG. 848 shows theabsorption vs wavelength for various device layer thickness ranging form120 nm to 400 nm. Curve 8410 is for 200 nm, curve 8412 is for 400 nm andcurve 8414 is for 120 nm. FIG. 84C shows absorption vs wavelength for adevice layer thickness of 70 nm.

In some cases, the microstructure holes in structures such asillustrated in FIGS. 83A and 84A can be aperiodic and/or random, and insome cases the microstructure holes can be any combination of periodic,aperiodic and/or random.

In some cases, the microstructure holes in structures such asillustrated in FIGS. 83A and 84A can be etched into the BOX layer, andin some cases through the BOX layer. In some cases, the dielectricfilling the microstructure holes can have a different refractive indexthan the BOX layer.

The thickness of the device layer in structures such as illustrated inFIGS. 83A and 84A can range from 30 nm to 500 nm, and in some cases from70 nm to 2000 nm. The BOX layer thickness can range from 50 nm to 2000nm. The microstructure hole lateral dimension can range from 300 nm to1000 nm, and in some cases from 400 nm to 1500 nm, and the spacingbetween adjacent holes can range from 100 nm to 1000 nm, and in somecases for conical shaped holes such as inverted pyramids, the spacingbetween adjacent holes can be toughing and/or overlapping. Themicrostructure holes can be circular, rectangular, polygonal, amoebic,and/or any combination of shapes.

In some cases, Ge and/or GeSi layer(s) with thickness ranging from30-500 nm can be epitaxially grown on the thin Si layer to extend thewavelength range beyond 1000 nm in structures such as illustrated inFIGS. 83A and 84A.

FIGS. 85A-B show partial simplified cross-sections of microstructureholes on a thin Si device layer. The device layer is on a SOI substratewhere the microstructure holes can be etched into and/or through the BOXlayer. FIG. 85A is similar to FIG. 83A with the exception that the holes8412 are etched into and/or through the BOX layer. FIG. 85B is similarFIG. 84A with the exception that the microstructure holes 8514 areetched into or through the BOX layer, and in some cases into the Silayer, and the microstructure holes can be filled with a dielectric thathave an index of a refraction different than the BOX layer, and in somecases can be filled with a dielectric with refractive index similar oridentical to the BOX layer. The dielectric can partially or fully fillthe microstructure holes, and in some cases multiple regions can havedifferent dielectric index such as in the case of partially filledholes.

In structures such as illustrated in FIGS. 83A and 84A on SOI wafers, insome cases the Si device layer can be partially or fully depleted, andthe device layer can be thin with thickness ranging from 5 nm to 200 nmand in some cases nm to 35 nm, and the BOX layer can have a thicknessranging from 10 nm to 200 nm and in some cases from 20 nm to 100 nm, andin some cases greater than 200 nm, and the handle substrate can beintrinsic, and in some cases can be lightly doped with thickness rangingfrom 1 micron to 700 microns, and in some cases 1 micron to 3 microns,and in some cases 3 microns to 5 microns.

The lateral dimension of the microstructure hole can be divided by theoptical refractive index of the material that fills the microstructurehole in some cases.

FIG. 86A shows a cross-section schematic of a microstructure holephotodetector. The device layer is etched to the BOX layer to form themicrostructure holes 8612, and the device layer can be removed in areaswhere Ge and/or GeSi growth are not desired, and in some areas, the Sidevice layer can be covered with a dielectric such as Si dioxide, or Sinitride for example where Ge and/or GeSi epitaxial growth are notdesired. Using selective area epitaxial growth of Ge and/or GeSi onexposed Si surfaces can form Ge/GeSi on Si photodetector withmicrostructure holes. P and N doping can be formed interdigitally andinterdigit M1 and M2 electrodes can make ohmic contact to the P and Nwells. The thickness of the Ge and/or GeSi layer can range from 20 nm to500 nm, and in some cases from 30 nm to 450 nm, and in some casesgreater than 500 nm. The microstructure holes 8612 can be periodic,and/or aperiodic and/or random and/or any combination thereof arranged.The lateral dimension of the microstructure hole can range from 400 nmto 1500 nm, and in some cases from 300 nm to 1500 nm, and the spacingbetween adjacent holes can range from 100 nm to 600 nm, and in somecases from 50 nm to 300 nm, and in some cases from 300 nm to 1000 nm. Insome cases, the spacing between the holes can range from ½ a wavelengthto 1 wavelength, and in some cases material, such as Ge and/or GeSi.Light can impinge from the top surface, and in some cases, light canimpinge from the bottom surface. In some cases, the selective areagrowth of the Ge on Si photodetector can be formed on the bottom surfaceor the handle wafer surface, and the CMOS and/or BiCMOS electronics canbe formed on the device layer. Such a device allows easy formation ofelectrical contacts with the CMOS and/or BiCMOS electronics, especiallyin the case of high-density arrays of photodetectors, which canbephotodiodes/APO/SPAD. The formation of ASICs electronics on the devicelayer and the photodetector arrays on opposing surfaces have beendescribed above see for example FIG. 58 to FIG. 64. FIG. 86A shows alateral PIN Ge/GeSi on Si microstructure hole photodetector where the Sidevice layer and the Ge/GeSi layer are I “intrinsic” or low dope P or N.A reverse bias is applied between the M1 anode, and the M2 cathode withreverse bias voltage ranging from 0.3 volts to 3.3 volts, and in somecases 3.3 volts to 35 volts, and some cases 35 to 50 volts. The incidentwavelength can range from 850 nm to 1100 nm, and in some cases from 900nm to 1350 nm, and in some cases from 1200 nm to 1650 nm, and in somecases from 1500 nm to 2200 nm.

FIG. 86B shows a cross-section schematic of a Ge/GeSi on Simicrostructure hole photodetector. The photo detector has a vertical PINstructure using selective area epitaxial growth similar to FIG. 86A. TheSi device layer can be doped fully or partially with a N+ well and acathode electrode can be formed in contact with the N+ well by etchingthrough the Ge and in some cases by forming a contact to the N+ wellseparate from the Ge/GeSi layer. The interdigits and in this case can beall anodes. The Ge/GeSi layer thickness and dimensions of themicrostructure holes are similar to FIG. 86a . A reverse bias voltage isapplied between the anode and cathode. The P and N can be interchanged.In some cases, portions of the Ge/GeSi layer can be N doped. In somecases, portions of the device layer can be P doped to form an avalanchediode in the Si, for example a PIPN structure, and in some cases a PNstructure.

FIG. 86C shows a Si microstructure hole vertical PIN where theinterdigits are anodes and the cathode electrode can be formed on the N+Si. The microstructure holes 8612 can be periodic, and/or aperiodic,and/or random, and any combination thereof arranged. The microstructureholes can have a lateral dimension ranging from 300 nm-1200 nm, and insome cases 400 nm-1000 nm, and the spacing between adjacent holes canrange from 100 nm-600 nm, and in some cases from 100 nm-1000 nm. In somecases, the adjacent holes can intersect for example in the case ofinverted pyramids. The thickness of the I or low dope Si can range from35 nm-1000 nm, and in some cases from 35 nm-400 nm. The N+ wellthickness can range from 10 nm-100 nm. A reverse bias is applied betweenthe anode and cathode with voltage ranging from 0.3 volts-35 volts. Thewavelength of the incident optical signal can range from 800 nm-1000 nm.

Data rates for data center interconnect applications in structures suchas illustrated in FIGS. 86A-C can range from 10 Gb/s-50 Gb/s, and insome cases to 100 Gb/s. Multiple photodetectors can be monolithicallyintegrated with

CMOS and/or BiCMOS ASICs and can be either on the front or back surfacesof the SOI wafer such that CMOS and BiCMOS ASICs and photodetectorarrays are on opposing surfaces. For LiDAR or flash LiDAR applicationsthe rise time of the microstructure hole photodetector in the 10-90% or20-80% rise time of the detected optical pulse can have a time responseof picoseconds for example 1-picoseconds, and in some cases 1-40picoseconds, and in some cases 5-picoseconds, and in some cases 10picoseconds or less. This gives a depth resolution of millimeters ascompared to commercial Si photodetectors with equivalent quantumefficiency of nanoseconds, or 10s of nanoseconds. For sensors such asCMOS image sensors with high density pixels, with pixel size of 1-25microns in lateral dimension the microstructure hole photodetectors canhave a higher IR sensitivity at certain wavelength than a comparableCMOS image sensor without microstructure holes. The microstructure holearray can be formed on the same surface as the CMOS ASICs, and in somecases the CMOS image sensor can be formed on the handle substrate or onthe opposing surface of the CMOS ASICs and where microstructure holescan be formed.

In some cases, in structures such as illustrated in FIG. 88A-C the I orlow dope Si can be N type and in some cases it can be low dope P type,and in some cases the anode electrode can be a Schottky contact. Areverse bias is applied between the Schottky metal contact and theburied N—Si layer.

FIG. 87 is a schematic top view of a vertical PIN photodetector. Thephotodetector can be Si as in FIG. 86C or Ge/GeSi on Si as in FIG. 86B,and where the photodetector(s) can be formed on the same surface as theCMOS and/or BiCMOS ASICs. The Ge/GeSi layer can be selective area grownand the anode can be a grid around the microstructure holes to reduceseries resistance, and the cathode can be formed on the N+ Si layer byetching a via through the Ge/GeSi layer, and the transmission linesconnected to the CMOS/BiCMOS ASICs. Other electrode configurations canbe used to optimized the performance of the photodetector.

FIGS. 88A-C show an FDTD simulation of the optical field impinging onthe top device layer surface. The “device layer surface” is of a 70 nmthick Si device layer on a 200 nm thick BOX layer structure as shown inFIG. 88A. The microstructure holes 8812 are circular and etched to theBOX layer, and arranged in a periodic square lattice, with diameterranging from 450 nm-1000 nm. The optical signal impinges normal to thesurface.

FIG. 88B shows the absorption vs wavelength where absorption is directlyproportional to external quantum efficiency for two differentmicrostructure hole diameters. The solid curve 8820 shows the case witha hole diameter of 1000 nm and a period of 1200 nm, the dashed curve8822 shows the case with a hole diameter of 900 nm and a period of 1200nm. The absorption is 40% or more over a wavelength range of 800-950 nm.

FIG. 88C shows absorption vs wavelength for the case of hole diameter of700 nm and period of 900 nm as solid curve 8830, and for hole diameterof 450 nm and period of 900 nm for the dashed curve 9932. Photodetectorswith microstructure holes can have a higher external quantum efficiencythan a comparable photodetector without microstructure holes at certainwavelengths.

FIGS. 89A-B show an FDTD simulation of a microstructure hole structure.FIG. 89A shows the configuration with microstructure holes 8912 formedin a 30 nm and 50 nm device layer thickness on a BOX layer of 200 nm.FIG. 89B shows the absorption vs wavelength for microstructure holedimensions of 900 nm diameter and 1200 nm period etched to the BOXlayer. The dotted curve 8924 shows absorption vs wavelength formicrostructure holes with device layer thickness of 50 nm, and the solidcurve 8922 for a device layer of 30 nm. The dashed curve 8920 shows theabsorption vs wavelength for 30 nm device layer thickness withoutmicrostructure holes.

FIGS. 90A-B show an FDTD simulation of the optical field of amicrostructure hole structure. FIG. 90A shows the configuration withmicrostructure holes 9012 formed in a device layer thickness of 30 nmand 60 nm and a dielectric such as Si dioxide of 70 nm and a BOX layerof 200 nm. The microstructure holes 9012 as in FIG. 89A have 900 nmdiameter, and 1200 nm period, and are etched to the BOX layer. In FIG.90B the solid curve 9022 is for microstructure holes with a dielectriclayer, and a device layer thickness of 30 nm. The dotted curve 9024 isfor microstructure holes with dialectic and a device layer thickness of60 nm. The dashed curve 9026 is for microstructure holes with dialecticand a device layer thickness of 30 nm. The dash-dot-dash curve 9020shows the absorption vs wavelength of a structure without microstructureholes and a device layer of 30 nm.

The dielectric on top of the Si device layer in FIG. 90A can have arefractive index similar to that of Si refractive index at a givenwavelength.

FIGS. 91A-B show an FDTD simulation of the optical field of amicrostructure configuration. The structure, shown in FIG. 91A, issimilar to the one in FIG. 90A except that the dielectric on top of theSi device layer can be Ti oxide or Hf oxide. The Si device layer is 30nm thick, and the Hf oxide or Ti oxide is 100 nm thick, and the BOXlayer is 200 nm on top of Si. In FIG. 91B the plots show absorption vswavelength where absorption can be directly proportional to externalquantum efficiency, and for wavelength ranging from 800-950 nm. Thedotted curve 9126 shows absorption vs wavelength for microstructureholes of 1200 nm in diameter, and 1500 nm period in a square latticewith Ti oxide dielectric on top of the device layer. Curve 9120 is for1000 nm diameter, 1200 nm period with Hf oxide, curve 9122 is for 1200nm diameter, 1500 period with Ti oxide, curve 9124 is for 1100 nmdiameter, 1400 nm period with Hf oxide, and curve 9128 is for 1000 nmdiameter holes, 1200 nm period with Ti oxide. The absorption in thisconfiguration is greater than 15% over the wavelength range of 800-950nm. A comparable structure without microstructure holes has absorptionof less than 1% over the same wavelength range.

FIG. 92 shows a partial cross-section schematic of a lateral PINinterdigitated photodiode. The photodiode is fabricated on a SOI waferwhere the Si device layer can be I or low dope P or N, and can bepartially or fully depleted, and can have thickness range of 8 nm-200nm, and in some cases 10-30 nm.

CMOS ASICs are formed on the Si device layer and can be monolithicallyintegrated with the lateral PIN photodiode which can have multiplephotodetectors, and in some cases a 2D array of photodetectors foroptical data communication, LiDAR, or 3D imaging. The lateral PIN can becovered with a high index dielectric such as Hf oxide, and can befurther covered with Si dioxide. Microstructure holes 9212 are formed inthe dielectric and can be etched to the BOX layer as shown in FIG. 92.Light can impinge on the top surface. The interdigitated electrodes canhave spacing ranging from 100 to 1000 nm, and the width of theinterdigits can range from 10 nm to 160 nm. The thickness of thedielectric which can have single or multiple layers of differentrefractive index can have thickness ranging from 50 nm to 600 nm. Thediameter of the microstructure holes can range from 400 nm-1200 nm. Themicrostructure holes can be periodic and/or aperiodic, and/or random,and can be circular, rectangular, polygonal in shape and can havespacing ranging from 200 nm to 1000 nm. Wavelength range for themicrostructure hole photodetector can range from 800 nm to 1100 nm, andin some cases from 800 nm to 1000 nm. The external quantum efficiency ofa microstructure hole photodetector can be greater than the externalquantum efficiency of a comparable photodetector without microstructureholes at certain wavelengths.

FIG. 93 shows a partial cross-section schematic of a lateral PINinterdigitated photodiode similar to FIG. 92. In the case of FIG. 93 themicrostructure holes 9312 are etched partially into one or moredielectrics, and not into the Si device layer. The external quantumefficiency of microstructure hole photodetector can be higher than theexternal quantum efficiency of a comparable photodetector withoutmicrostructure holes at certain wavelengths.

FIG. 94 is a schematic of a top view of microstructure lateral PIN asshown in FIGS. 92 and 93. Only a single photodetector is shown forsimplicity. Multiple photodetectors in 1D or 2D arrays can be fabricatedon a single chip and monolithically integrated with CMOS ASICs. In thisstructure the interdigits are first formed followed by the etching ofmicrostructure holes 9412 in the dielectric that can be partially etchedinto the dielectrics, or through the dielectrics to the Si device layer,or to the BOX layer. The microstructure holes 9412 can have a largerlateral dimension than the spacing of the interdigit electrodes.Transmission lines connecting the M1 and M2 interdigits are connected toa CMOS ASICs.

A reverse bias voltage is applied to the M1 anode, and M2 cathode inFIG. 94 with voltage ranging from 0.1 volt to 4 volts, and in some casesgreater than 4 volt, where multiplication gain is desired.

FIG. 95 shows a simplified partial cross-section schematic of a bottomilluminated CMOS image sensor or a bottom illuminated CMOS high speedvertical PIN photodiode for optical data center interconnectapplications or for LiDAR or Time-of-Flight, or for Time-of-Flight 3Dimaging. The CMOS ASICs are formed in the Si device layer of a SOI waferthat can be partially or fully depleted, and in some cases not partiallyor fully depleted, and the photodetector is formed on the oppositesurface on the handle substrate where the handle substrate can bethinned to 5 micron thickness or less, and in some cases to 2 micronthickness or less. P and N junctions can be formed by ion implantationfollowed by rapid thermal anneal and microstructure holes can be etchedto the BOX layer. The handle substrate 9506 can be I or low dope N or P,and the P and N can be interchanged. Electrodes are connected from thetop CMOS ASICs to the P and N layer of the photodetector by means of avia. The lateral dimension of the photodetector or pixel can range from1 micron to 25 microns, and in some cases 25 microns-50 microns, and insome cases more than 50 microns. Microstructure holes 9512 lateraldimensions can range from 300 nm to 1200 nm, and in some cases 600nm-1000 nm, and in some cases greater than 1200 nm. The spacing betweenadjacent holes can range from 100 nm to 600 nm, and in some cases theholes can touch or intersect if the holes are inverted pyramids forexample. Isolation trenches 9530 can be included to separate thephotodetector or pixel. For data communication, the data rate can rangefrom 10-50 Gb/s, and in some cases 50-100 Gb/s, and in some casesgreater than 100 Gb/s. The rise time for Time-of-Flight applications canrange from 1 picosecond to 30 picoseconds, and in some cases from 10picosecond to 40 picoseconds, and in some cases less than 100picoseconds. The external quantum efficiency of a microstructure holephotodetector can be greater than the external quantum efficiency of acomparable photodetector without microstructure holes at certainwavelengths, the microstructure holes 9512 can be periodic, and/oraperiodic, and/or random. Optical signal and/or time of flight signaland/or images impinge on the bottom surface. A reverse bias is appliedbetween the anode 9520 and cathode 9522 with voltage ranging from 0.1 to4 volts, and in some cases greater than 4 volts where multiplicationgain is desired. Wavelength range from 800-1100 nm.

FIG. 96 shows a simplified partial cross-section schematic of a bottomilluminated CMOS image sensor or a bottom illuminated CMOS high speedvertical PIN photodiode. FIG. 96 is similar to FIG. 95 with the additionof selective area growth of Ge 9604 on Si 9606. The P layer is formed onGe 9604 and the N layer is formed on Si 9606. The Ge and/or GeSi layercan have a thickness ranging from nm to 500 nm, and in some cases 50nm-400 nm. The Ge or GeSi can I or low dope P or N. The microstructureholes 9612 can be periodic, aperiodic, and/or random, and/or anycombination thereof. The microstructure holes can be partially etchedinto the Ge layer and in some cases etched to the Si layer and in somecases etched to the BOX layer. The lateral dimension of themicrostructure hole can range from 300 to 1500 nm, and in some casesfrom 600 to 1500 nm, and in some cases more than 1500 nm. The spacingbetween adjacent holes can range from 100 nm to 600 nm, and in somecases greater than 600 nm. The lateral dimension of the photodetectorcan range from 2 microns to 30 microns, and in some cases from 30microns to 100 microns, and in some cases greater than 100 microns.Electrodes are formed connecting the anode and cathode to the CMOSASICs, and a reverse bias can be applied between the anode and cathodewith voltage ranging from 0.1 to 4 volts, and greater than 4 volts wheremultiplication gain is desired. Wavelength range for the photodetectorcan be from 800 to 1650 nm, and in some cases from 800 to 1100 nm, andin some cases 800-1350 nm. Data rate can range from 10 to 50 Gb/s, andin some cases 50-100 Gb/s, and in some cases greater than 100 Gb/s foroptical interconnect application. Rise time can range from 1 to 20 picoseconds, and in some cases from 10-40 pico seconds, and in some casesless than 100 pico seconds for time-of-flight applications such as LiDARand 3D imaging. Microstructure holes photodetector can have externalquantum efficiency greater than the external quantum efficiency of amcomparable photodetector without microstructure holes at certainwavelengths. Optical signal and/or time-of-flight signal and/or 3Dimages impinge on the bottom surface. Multiple photodetectors/pixels canbe formed in 1D or 2D arrays that are monolithically integrated withCMOS ASICs.

FIGS. 97A-B are partial schematic cross-sections similar to FIG. 95. Inthe case of FIG. 97A, a lateral PIN configuration interdigitatedelectrodes M1 and M2 form alternating PN junctions. The width of the M1and M2 electrodes can range from 10 nm to 300 nm. The M1 and M2electrodes form ohmic contacts to the P and N doped wells which can beformed by dopant diffusion and/or ion implantation. The lateralphotodiode can be connected to the CMOS or BiCMOS ASICs by electrodes9720 and 9722 connecting the P and N regions respectively to appropriatecontacts in the ASICs electronics by means of a via. The lateraldimension of the photodetector can range from a few microns to 10s ofmicrons, and in some cases to 100s of microns. Applications can includeoptical interconnect for data centers, LiDAR for autonomous vehicles,robots, and drones and 3D imaging with or without time-of-flight.Multiple photodetectors and/or high density arrays can be fabricated andmonolithically integrated with CMOS/BiCMOS ASICs. A reverse bias isapplied between the anode and cathode with voltage ranging from 0.1 to 4volts, and in some cases 4-50 volts where multiplication gain indesired.

FIG. 97B is similar to FIG. 97A without the M1 or M2 interdigitatedelectrodes, where the N and P doping are sufficiently high such thatelectrodes may not be necessary. A reverse bias is applied between theanode and cathode with voltage ranging from 0.1 to 4 volts, and in somecases 4-50 volts where multiplication gain in desired.

FIGS. 98A-B are partial schematic cross-sections similar to FIG. 96. Inthe case of FIG. 98A, a lateral PIN structure has interdigitated M1 andM2 electrodes on alternating P and N junctions. Connections of thephotodetector anode and cathode to the CMOS electronics are made withelectrodes 9820 and 9822 passing through a via in the BOX layer andlayers in the photodetector to connect to the P and N ohmic contacts. Areverse bias is applied between the anode and cathode with voltageranging from 0.1 ro 4 volts, and in some cases 4-50 volts wheremultiplication gain in desired. The detector can detect light or opticalsignal with wavelength ranging from 800 ro 1650 nm, and in some cases to2200 nm, and in some cases 850 nm-1100 nm, and in some cases 1200nm-1350 nm, and in some cases 850 nm-1550 nm. Applications includeoptical interconnect for data centers, LiDAR for autonomous vehicles,robots, and drones, 3D imaging with or without time-of-flight.

FIG. 98B is similar to FIG. 98A without the metal M1 and M2interdigitated electrodes. In some cases, silicide such as Pt, Ti or Alsilicide can be used in place of the metal electrodes, and in some casesthe highly doped P and N region have sufficiently low series resistancefor certain applications such that interdigtated metal electrodes maynot be necessary.

All or almost all of the photodetector structures discussed in thispatent specification, and/or the commonly assigned incorporatedapplications can be fabricated on the back side of a SOI wafer and theCMOS and/or BiCMOS electronics can be fabricated on the front side(device layer side).

In all cases for embodiments according to this patent specification themicrostructure holes can be passivated with thermal native oxide and/orother dielectrics such as Al oxide, Si nitride, Hf oxide, to name a fewby methods such as atomic layer deposition, and/or in some cases themicrostructure holes can be partially or entirely filled with Si dioxideand/or other dielectrics. In addition, the Si dioxide, and/or otherdielectrics can fill the microstructure holes and extend beyond theholes onto the surface. In some cases, the passivation layer for themicrostructure holes can be amorphous semiconductor such as amorphousSi, and/or amorphous Ge to name a few.

Avalanche photodiode and/or single photon avalanche photodiode can alsobe fabricated in the back illuminated photodetector array in structuresaccording to embodiments described in this patent specification withappropriate P N junction doping profiles and in some cases PIPN, and insome cases PIPIN, and where in some cases the P and N can beinterchanged for both Si and Ge on Si structures.

FIGS. 99A-B show an FDTD simulation of optical fields that are absorbedin a thin Si layer on top of a BOX layer in a SOI structure. Across-section schematic is shown in FIG. 99A. Al electrodes are placedon the thin Si layer of 40 nm thickness, the Al has a width of 200 nmand a thickness of 20 nm. The structure is covered with HfO₂ to athickness of 1000 nm. Holes 9912 are arranged in a square lattice areetched through the HfO₂ to the BOX layer with diameter of 800 nm and aperiod of 1000 nm. The FDTD simulation was made for both the opticalelectric field parallel and perpendicular to the interdigit Alelectrodes. FIG. 99B plots absorption which is directly proportional toexternal quantum efficiency for wavelength ranging form 800-950 nm. Thesolid curve 9920 is for the case without electrodes, and the dashedcurve 9924 is for the case with electrodes, and where the opticalelectric field is perpendicular to the interdigitated electrodes. Thedotted curve 9922 is for the case with electrodes, and where the opticalelectric field is parallel to the interdigitated electrodes, and thedash-dot-dash curve 9926 is for the case with electrodes with bothoptical electric field parallel and perpendicular to the electrodes. Ascan be seen the absorption or quantum efficiency can range as high as50% at 800 nm wavelength to over 20% quantum efficiency at 950 nm.

Photodetectors with microstructure holes can have a higher externalquantum efficiency than a comparable photodetector withoutmicrostructure holes at certain wavelengths.

FIGS. 100A-B are partial schematic cross-sections of structure similarto that shown in FIG. 99A. In the case of FIG. 100A, P and N wells areadded within the 40 nm thick Si layer 10010. The microstructure holes10012 are etched through the dielectric (HfO₂) to the BOX layer. And insome cases, the holes can be partially etched into the dielectric, andin some cases the holes can be etched to the Si device layer.

FIG. 100B is similar to FIG. 100A but with the lateral dimension of themicrostructure hole 10014 wider than the spacing of the electrodes, asshown in this case the microstructure hole 10014 etched through thedielectric to the device layer, and in some cases etched partially inthe dielectric layer, and in some cases etched into the device layer,and in some cases etched to the BOX layer, and in some cases etched intoor through the BOX layer.

The width of the Al electrodes in structures such as illustrated inFIGS. 100A-B can range from 40 nm to 300 nm, the spacing between the Alelectrodes can range from 100 nm to 1000 nm, and in some cases more than1000 nm. The thickness of the Al electrodes can range from 10 nm to 100nm, and in some cases more than 100 nm, and the length of the Alelectrodes can range from 1 micron to 1000 microns or more. Theelectrode can be other metals such as Cu, Mo, Ta, Pt, to name a few, andin some cases the electrodes can be metal silicide, and in some casesthe electrode can be heavily doped P or N semiconductor regions. Thedielectric holes lateral dimension can range from 300 nm to 1600 nm, thedielectric thickness can range from 100 nm to 2000 nm or more, and thedielectric can be Ti oxide, Hf oxide, Si nitride, Si dioxide, to name afew. As in previously discussed structures with appropriate P and Ndoping profile and with PN, PIN, PIPN, PIPIN avalanche photodiodes,single photon avalanche photodiodes can be fabricated. Reference,Piemonte el. al, Overview on the main parameters and technology ofmodern Silicon Photomultipliers, Nuclear Inst. and Methods in PhysicsResearch, A 926 (2019)2-15

As shown in FIG. 99B with and without the interdigit electrodes underthe dielectric absorption over a wavelength range of 800-950 nm isapproximately the same. It can be seen that the geometric blocking ofthe optical signal by the electrode is minimal since the electrodes aresubwavelength in the width dimension. This structure is different fromprior art which doesn't include the electrode under the dielectrics.

The thickness of the dielectric in structures such as illustrated inFIGS. 100A-B can range from 100 nm to 1000 nm and in some cases greaterthan 1000 nm. The microholes in the dialectic can be filled partially orfully or buried by another dielectric with a different refractive index,and the dielectric on which the microholes are formed. The electrodesand/or P and N wells in some cases can be aligned with the microholes asshown in FIG. 100, and in some cases the electrode and/or P and N wellsneed not be aligned with the microholes. For example, the electrodeand/or P and N wells can be intersecting with the microholes.

FIGS. 101A-B show an FDTD simulation of surface illuminated opticalfield of a structure. FIG. 101A shows the simulated configuration. AnSOI wafer with 200 nm BOX layer and 30 nm Si device layer 10110 and withdielectric such as Hf oxide of 110 nm thick deposited on the Si devicelayer 10110. Metal interdigitated electrodes can be buried under the Hfoxide as shown in FIGS. 100A-B. The interdigits electrodes can be metal,silicide, heavily doped regions, transparent metal oxides to name a few.The microstructure holes 10112 are circular with a diameter of 800 nmand a period of 1000 nm in a square lattice. The holes can be periodic,aperiodic, and/or random and/or any combination thereof. Light impingeson the top surface or the dielectric surface. In FIG. 101B, curve 10122is for a configuration without microstructure holes and the absorptionis less than 1% for wavelength range of 800-950 nm. With Hf oxide shownby the dotted curve 10124 the structure can have an absorption which isdirectly proportional to quantum efficiency and is between 40-60% overthe wavelength range. Without the dielectric (curve 10120), theabsorption is roughly 20% in the wavelength range. Microstructure holephotodetector can have a higher external quantum efficiency than acomparable photodetector without microstructure holes at certainwavelengths.

FIGS. 102A-B shows an FDTD simulation of surface illuminated opticalfield of a structure. The structure shown in FIG. 102A is similar to thestructure shown in FIG. 101A except that the holes 10212 are etched tothe Si device layer. Electrodes can be buried underneath the dielectricas in FIG. 100A-B and as in FIG. 99A the electrodes will have minimaleffect on the absorption. FIG. 102B shows the plotted FDTD simulation.The absorption efficiency can range from 50-60% over the wavelengthrange of 800-950 nm. Curve 10220 is for holes etched to the SiO2 layerwhile curve 10224 is for holes etched to the Si layer. Curve 1022 is fora structure without holes.

FIGS. 103A-C shows an FDTD simulation of surface illuminated opticalfield of a structure. The structures, shown in FIGS. 103A and 103B aresimilar to that shown in FIG. 102A. The holes are etched to the devicelayer and are rectangular with a lateral dimension of 800 nm and periodof 1000 nm with a conical shape in the case of holes 10312 formed in a250 nm Hf oxide layer 10310, as shown in FIG. 103A. FIG. 103B showsrectangular holes 10314 that are trapezoidal in Hf oxide layer 10310that is 110 nm thick. In FIG. 103C, the solid curve 10320 gives thetrapezoidal holes with 110 nm of dielectric has absorption ofapproximately 20% over the wavelength range of 800-950 nm. The conicalor inverted pyramid holes on 250 nm (curve 10324) has approximately30-40% absorption over the wavelength range of 800-950 nm. Absorption isdirectly proportional to external quantum efficiency and if all thephotogenerated carriers are collected the absorption can be equal toexternal quantum efficiency. Curve 10326 is for a cylindrical holes, 800nm diameter, 1000 nm period, square lattice, etched to the Si substratethrough 250 nm HfO2, 30 nm Si, 200 nm BOX. Curve 10322 is for justcylindrical holes 800 nm diameter, 1000 nm period in 30 nm Si.

Very thin Si device layer of 10-30 nm and in some cases 10-100 nm areoften used in current state of the art CMOS technology where NMOS andPMOS are formed on these thin Si device layer. In some cases, the thinSi device layer can be partially or fully depleted, and often is a lowdope P layer, and in some cases it can be a low dope N layer.

Photodiodes, avalanche photodiodes, and/or single photon avalanchephotodiodes 1D or 2D arrays according to the embodiments described inthis patent specification can be formed on the thin Si layer withappropriate P and N doping in a lateral PIN, PIPN, PIPIN structure. Insome cases the holes can be fully or partially filled with a dielectricof a lower index than the dielectric where the holes are formed. In somecases, the holes can be partially or fully filled with a dielectric witha higher index than the dielectric on which the holes are formed. Insome cases, the holes can be fully buried with a dielectric with arefractive index that is different than the refractive index of thedielectric in which the holes are formed. Optical fields impinge on thetop surface or the dielectric surface, and in some cases can impingefrom the bottom surface through a via in the Si handle layer.

FIGS. 104A-H are a simplified partial schematic of a top views ofphotodetector arrays configured as dense 2D arrays for imagingapplications. In FIG. 104A, each pixel can have lateral dimensionsranging from 1000 nm to 2000 nm. In the case for pixels of 1000-2000 nmlateral dimension the number of microholes can range from 1 to 10 ormore, and in some cases only 1 microhole may be formed in each pixel.The dimension of the microhole is approximately a wavelength, forexample 600-1000 nm, and in some cases 700-900 nm.

In FIG. 104B, a single microhole is shown in a pixel where the distancebetween the edge of the microhole to the edge of the pixel can beapproximately 1 wavelength in the material (free spacewavelength/refractive index of material), for example can havedimensions ranging from 200 to 500 nm. Each pixel can be isolated fromthe adjacent pixel with an isolation trench that can extend partiallyinto the Si and in some cases can extend to the BOX layer.

FIG. 104C shows a single microstructure hole in a pixel where themicrostructure hole is an inverted pyramid that can be formed with wetetching.

FIGS. 104D-E show multiple microholes in a pixel with larger lateraldimension.

FIGS. 104F-G show microholes of different lateral dimensions within asingle pixel. FIG. 104H shows a single microhole in a pixel where themicrohole is random, freeform or “amoeba” shaped.

Not shown in FIGS. 104A-H are the connecting metal layers or electrodesor metal silicide connecting the pixels to CMOS electronics. In somecases the pixels can have a common connection on the surface andindividual connection to each pixel by means of an electrode passingthrough the BOX layer and connecting to the CMOS electronics on theopposing surface.

The photosensor arrays in FIGS. 104A-H can be 1000×1000 pixels, and insome cases can be 10,000×10,000 pixels or more, and in some cases can beless than 1000×1000 pixel array. The photosensor can be a photodiodeand/or avalanche photodiode and/or single photon avalanche photodiode,and can have wavelength range from 700 to 1000 nm, and with an additionof Ge or GeSi alloy the wavelength range can be extended to 1650 nm. Inthe case of large pixels microhole arrays can range from 10×10 to1,000×1,000 or more microholes. The microholes can be periodic and/oraperiodic and/or randomly arranged. The photosensor with microholes andhave a higher external quantum efficiency than a comparable photosensorwithout microholes at certain wavelength in the range of 700-1650 nm. Intime-of-flight applications the microhole photosensors can have risetime in the 10s of pico seconds.

FIGS. 105A-C shows simplified partial cross-sections of a singlemicrostructure hole in a pixel. CMOS electronics are shown on theopposing surface, and not shown are the connecting electrodes passingthrough the BOX layer, connecting each pixel to the CMOS electronics. InFIG. 105A, the P layer can be formed followed by dry etching of themicroholes 10512 partially into the Si layer, and followed by theformation of N layer at the bottom of the microhole 10512. The P and Nlayers can be formed by ion implantation. In this example the ionimplantation energy can be low since the ion does not have to penetratethe entire depth of the Si. The P and N regions can be interchanged.Isolation trenches 10530 can be etched partially into the Si, and asshown can be etched to the BOX layer. The isolation trenches 10530 andmicroholes 10512 can be filled with a dielectric such as SiO₂, and thesurface can be planarized using chemical mechanical polishing forexample and a common electrode can be formed on the P surface for allthe pixels. The thickness of the Si layer on which photosensors areformed can have a thickness ranging from 1000-5000 nm, and in some casesto 10,000 nm. In some cases, the thickness of the Si on which thephotosensors are formed can have thickness ranging from 100 nm-5000 nm,and in some cases less than 100 nm.

FIG. 105B shows a simplified partial cross-section schematic of a pixelwith a single microhole 10514 in this case an inverted pyramid. P and Nregions can be formed by ion implantation and the inverted pyramid canwet etched. Isolation trench 10534 can be formed to isolate each pixelelectrically and/or optically. As in FIG. 105A the trenches in themicroholes can be buried with an oxide. The oxide can also serve as apassivation layer. Not shown are connecting electrodes of each pixel tothe CMOS electronics by means of a via through the BOX layer. N regionof the pixels can be a common electrode.

FIG. 105C is similar to FIG. 105B except that the inverted pyramid 10514is formed first followed by an N dopant which can be diffused and/or ionimplanted. As in FIGS. 105A-B the trenches and the microholes can beburied with an oxide. The lateral dimension of the inverted pyramid canbe approximately a wavelength for example 700-1000 nm and the distancefrom the edge of the pyramid to the edge of the pixel can be 1wavelength in the material for example 200-500 nm. Light or opticalsignal or optical image impinge on the surface with the microholes. Thewavelength can range from 700-1100 nm for Si and with the addition of Geor GeSi alloy the wavelength can range from 700-2100 nm. The photosensorcan be a photodiode or avalanche photodiode, or single photon avalanchephotodiode, and can have rise time in the 10s of pico seconds, and canhave bandwidth ranging from 1 GHz to 100 GHz, and in some cases lessthan 1 GHz. Optical image or signal impinge on the surface withmicroholes and is surface illuminated. The devices shown in FIGS. 105A-Care sometimes known as back illuminated CMOS image sensors.

With appropriate doping profiles of P and N junctions, and in some casesPIN, and in some cases PIPN, and in some cases PIPIN (P and N can beinterchanged in structures such as illustrated in FIGS. 105A-C. Howeverfor the lowest noise APD/SPAD ionization of electrons for avalanche gainis preferred). The pixels with microholes can be photodiode (PD) and/oravalanche photodiode (APD) and/or single photon avalanche photodiode(SPAD)

FIG. 106 shows experimental results of absorption enhancement withmicrostructure holes or microholes in structures such as illustrated inFIG. 47C and in other new lateral Schottky MSM structures described inthis patent specification. Absorption coefficient vs wavelength isplotted for various material such as Si, and GaAs without microholes ascompared with Si MSM photodiode with microholes and Si PIN verticalstructure photodiode with microholes. The curve 10620 with large dotsare experimental results of Si MSM interdigitated lateral photodiodewith microstructure holes or microholes where the effective absorptioncoefficient at 850 nm wavelength is enhanced by 35 times to an effectiveabsorption coefficient of 18,000 cm⁻¹ as compared to the absorptioncoefficient of Si without microstructure holes of 535 cm⁻¹. At 850 nmwavelength GaAs without microholes has an absorption coefficient ofapproximately 12,000 cm⁻¹. This is the first time that with photontrapping using microholes that absorption and/or quantum efficiency ofSi is greater than that of GaAs at the wavelength range of 850 nm-980nm.

The Si MSM lateral interdigitated photodiode with microholes fabricatedon SOI Si wafer with device layer of 1 micron thickness and BOX layer of2 micron thickness achieve 85% external quantum efficiency at 850 nmexperimentally with a reverse bias (in MSM structures the currentvoltage is approximately symmetric and the device can operated in eitherreverse or forward bias, e.g., in structures such as illustrated in FIG.47C and in other new lateral MSM structures where both M1 and M2 areSchottky contacts as described in this patent specification). Comparablephotodetector without microstructure holes will have a lower EQEapproximately 10% or less. The microholes are approximately 1 wavelengthand the spacing between the microholes are approximately 1 wavelength inthe material in a square lattice, and the interdigitated electrode widthis approximately 300 nm with a spacing of approximately 1,000 nm.

A Schottky interdigitated MSM photodiode on SOI wafer with 1 microndevice layer with a resistivity ranging from 1-10 ohm-cm, and withcylindrical holes with diameter ranging from 700 nm-1000 nm and with aspacing between the holes of 300 nm in a square lattice havedemonstrated experimentally an enhancement of the absorption coefficientby 35× at 850 nm wavelength and 37× at 905 nm wavelength as shown by thecircle. Such enhancement pertains to structures such as illustrated inFIG. 47C and to other new lateral Schottky MSM structures described inthis patent specification

FIGS. 107A-C show simplified partial schematic of a top views and across-section of a pixel with a single microstructure hole. The pixelcan be formed on the back side for example as in the case of backilluminated CMOS image sensor (BI-CIS) or it can be formed on the topsurface for a front illuminated CMOS image sensor (FI-CIS). The lateraldimension of the pixel can range from 1 to 5 microns. With proper dopingprofiles such as PN, PIN, PIPN for example the pixel can operate in thephotodiode or avalanche photodiode, or single photon avalanchephotodiode mode with proper reverse bias. The reverse bias voltage canrange from 0.3 V to 40 V, and in some cases 0.3 V 3.3 V, and in somecases from 3.3 V-15 V, and in some cases from 3.3 V-35 V.

FIG. 107A shows a top view of a pixel array where each pixel has asingle microstructure hole and each pixel can be isolated electricallyand optically with an isolation trench that can be etched partially orfully to the BOX layer (see trenches 10730 and 10732 in FIG. 107C). Inaddition, the trench and the microstructure hole can be filled with adielectric such as Si dioxide. Not shown are connecting electrodesconnecting the surface dopant region to adjacent pixels to form a commoncontact. In some cases, each pixel can have its own anode and cathode,and not have a common cathode for example. Light signal that can bemodulated optical signal for data communication for optical signal fromtime-of-flight applications or optical images impinges on the surfacewhere the holes are formed.

FIG. 107B shows a single pixel with examples of doping. A microstructurehole 10712 is formed within the pixel with a lateral dimension rangingfrom 600 nm-1300 nm, and in some cases 400 nm-1300 nm, and in some cases700 nm-1000 nm. The microstructure hole can be formed using dry etchingand can be circular, oval, rectangular, polygonal, amoebic to name afew. The microstructure hole can also be wet etched using TMAH to forminverted pyramids. The microstructure hole 10712 can be etched partiallyinto the Si or entirely to the BOX layer. Doping can be diffused and/orion implanted such that P dopant into the walls of the microstructurehole and an N dopant can be diffused or implanted surrounding the Pdopant for example. The N and P can be interchanged by appropriatedoping profiles of the P and N the device can operated in PD, APD, SPADmode.

FIG. 107C shows a simplified partial schematic cross-section of a singlemicrostructure hole within the pixel where the microstructure hole 10712is shown as cylindrical and partially etched into the Si, and a P dopantis formed along the wall and the bottom of the hole, and an N dopant isformed adjacent to the P dopant. The thickness of the Si layer can rangefrom 100 nm to 3000 nm, and in some cases can range from 300 nm to 3000nm, and in some cases can range from 30 nm to 300 nm. The Si can be I orlow dope N or P. In some cases, GeSi or Ge layers can be grown on the Sito form a Si/GeSi/Ge layer on which the single microstructure hole canbe formed. Hole 10712 extends down into the P-type material, which inturn is surrounded by the I-region, so in effect the hole extends intothe I-region as well. The depth of the hole can be grater than the depthof an inverted pyramid etched into a single-crystal semiconductor giventhe semiconductor's inherent crystal planes. Connecting electrode 10720connects the P region (anode) to the CMOS electronics and commonelectrodes 10722 and 10724 connect adjacent electrodes; for example thecathode can be formed as shown and these electrodes can be connected toCMOS electronics which is not shown. In some cases, each pixel can havethe anode and cathode connected directly to the CMOS electronics. Theexample shown in FIG. 107C is a BI-CIS where the CMOS electronics andthe detector are on opposite sides of the BOX layer.

In some cases, the lateral dimension of the microstructure holes can beapproximately the nominal wavelength in free space divided by theoptical refractive index of the material that fills the microstructureholes.

FIGS. 108A-C show an FDTD simulation of a thin Si device layer on SOIsubstrate (as in FIGS. 108A-B) where the Si is 30 nm thick, the BOXlayer is 100 nm on Si substrate. The electrodes 10820 in FIG. 108A and10824 in FIG. 108B are buried under the HfO₂ layer 10810. Conical holes10812 are formed on the HfO₂ 10810 which has a thickness of 250 nm. Theelectrodes formed on the Si are 300 nm wide, 50 nm thick, and 100microns long. The lateral dimension of the conical holes 10812 which istriangular shaped is 800 nm with a period of 1000 nm in a squarelattice. The electrodes can be under the hole, or not under the hole. Asshown in FIG. 108C with the dotted curve 10834 where the electrodes areunder the hole, the dashed cure 10832 where the electrodes are betweenthe holes, and the solid line 10830 is without any electrodes. As shownin the calculations for wavelength 800 nm-950 nm the difference betweenthe 3 sets of curves is less than 5%, and has an absorption greater thanor equal to 30% over the wavelength range. In some cases, the absorptioncan be greater or equal to 20% at certain wavelength range. Aphotodetector with microstructure hole or holes can have a higherexternal quantum efficiency than a comparable photodetector withoutmicrostructure hole/holes at certain wavelengths in the range of 800 nm950 nm.

FIG. 109 shows a partial schematic cross-section of a light trappingstructure. Micro-holes 10914 are etched into the active layer that canbe Si/GeSi/Ge and the microstructure holes can be filled with adielectric such as SiO₂, and in addition the oxide can extend by 100nm-3000 nm thick and on which additional microstructure holes 10912 canbe formed. Not shown are electrodes for vertical PIN, PN, PIPN, PIPINphotodetector or electrodes for lateral PN, PIN, PIPN photodetectorwhich can be PD or APD or SPAD. Optical signal impinges on the topsurface with the microstructure holes 10912. The BOX layer can beoptional and can have a thickness ranging from 20 nm to 2000 nm or more,the Si device layer can have a thickness ranging from 10 nm to 1000 nmand the GeSi/Ge layer can have a thickness ranging from 100 nm to 1000nm that can be grown epitaxially on the Si device layer, and in somecases can be grown using selective area epitaxy growth. Themicrostructure holes 10914 formed in the Si/GeSi/Ge can have lateraldimension ranging from 300 nm to 1300 nm, and in some cases 500 nm-1000nm, and the spacing between the microstructure holes 10914 can rangefrom 100 nm to 500 nm, and in some cases more than 500 nm. The depth ofthe microstructure holes 10914 can be partially etched into theSi/GeSi/Ge or entirely to the BOX layer, in the case of no BOX layer tothe Si substrate. The microstructure holes 10914 in the Si/GeSi/Ge canhave a cylindrical cross-section, and in some cases a conicalcross-section, and in some cases an inverted pyramid to name a few. Theoxide can partially or entirely fill the microstructure holes 10914, andcan extend to a thickness ranging from 100 nm to 5000 nm. In some casesa thin layer of amorphous Si can be formed on the side walls of theGeSi/Ge microstructure holes for passivation prior to depositingdielectric such as SiO₂. Microstructure holes 10912 can be formed on theSiO₂ or dielectric that can be coincidental with the microstructureholes 10914 in the Si/GeSi/Ge. And in some cases, the microstructureholes 10912 in the dielectric need not be coincidental.

The additional microstructure holes 10912 in the dialectic can havelateral dimension larger than the lateral dimension of microstructureholes in the Si/GeSi/Ge. The additional microstructure hole 10912 in thedielectric help reduce reflection from the surface and help funneltrapped photons to the microstructure holes in the semiconductor.

The lateral dimension of microstructure holes 10912 is approximately awavelength, and the spacing between the microstructure holes isapproximately a wavelength in the material. The wavelength can be themean wavelength of the incident signal spectrum for example. In somecases, the lateral dimension can be less than a wavelength for examplewavelength/2 and in some cases more than a wavelength were wavelength xinteger.

The lateral dimension of microstructure holes in most cases mentioned inthis patent specification are that for microstructure holes not filledwith any dielectric, and filled only with air or vacuum where theoptical refractive index is approximately 1. In the cases where themicrostructure holes are filled fully or partially with the dielectricthe lateral dimension of the microstructure hole can be reduced by theeffective optical refractive index of the dielectric/voids in themicrostructure holes. For example, a microstructure hole with lateraldimension of 800 nm not filled in air can have a lateral dimension of533 nm if it was completely filled with SiO₂ which has an opticalrefractive index of approximately 1.5. Microstructure hole lateraldimension can in some cases be reduced when it is filled with dialectic,where the refractive index is greater than 1 for example (lateraldimension of microstructure hole in vacuum or air)/(optical refractiveindex), and in some cases where the microstructure hole is partiallyfilled with dielectric and effective optical refractive index can becalculated by the ratio of the volume of 1 or more dielectrics in themicrostructure hole.

FIGS. 110A-C show FDTD simulated optical absorption, reflection andtransmission of a single hole pixel in Si on a BOX layer, according tosome embodiments. As shown in FIGS. 101A and 101B, the pixel size is1300 nm square and the microstructure hole 11012 is 800 nm in diameterand is etched to the BOX layer. The thickness of the Si is 1 micron. InFIG. 101C, the simulation shows that the absorption which isproportional to the external quantum efficiency can be 50% or more inthe wavelength range 800-950 nm. In some cases, the absorption can be ashigh as 80% at certain wavelengths. The solid curve 11020 is absorption,the dash curve is reflection and the dotted curve is transmission. Thesecurves are related by the equation A+R+T=1 where A is absorption, R isreflection and T is transmission for this FDTD simulation of the opticalfields incident at a normal and/or almost normal (+/−15 degrees) angleto the single microstructure hole pixel shown in FIG. 110A-B. Externalquantum efficiency, EQE, is proportional to absorption. If all the photogenerated carriers are collected by the anode and cathode that are inturn connected to an external circuit that can include voltage bias, andsignal processing ASICs convert the photo generated carriers into anelectrical signal, the EQE can equal absorption and can be 50% or moreat certain wavelengths in the range 800-950 nm and in some cases to 1000nm. If any photogenerated carriers are lost to recombination for examplethe EQE will be less that absorption and in some cases 10-20% less andin some cases 20-50% less and in some cases 50-60% less at certainwavelengths in the wavelength range 800-950 nm and in some cases to 1100nm. Pixels with microstructure hole(s) can have a higher EQE than pixelwithout microstructure hole(s) at certain wavelengths. The simulation isof single hole pixel where the hole is not filled with any dielectricexcept air. In some cases, the diameter of the microstructure hole canbe reduced if the hole is filled or partially filled or buried by adielectric. The diameter can then be given approximately by the diameterin free space divided by the optical refractive index of the dielectricmaterial. In some cases, as in FIG. 109, additional microstructure holescan be formed in the dielectric to reduce reflection from the dielectricsurface and improve light absorption in the microstructure holes Si. Thepixel can be isolated from adjacent pixels by a trench that can befilled with a dielectric. The number of pixels can range from 100×100 to1000×1000 to 5000×5000 or more.

Although the foregoing has been described in some detail for purposes ofclarity, it will be apparent that certain changes and modifications maybe made without departing from the principles thereof. It should benoted that there are many alternative ways of implementing both theprocesses and apparatuses described herein. Accordingly, the presentembodiments are to be considered as illustrative and not restrictive,and the body of work described herein is not to be limited to thedetails given herein, which may be modified within the scope andequivalents of the appended claims.

1. An integrated, single-chip structure comprising a photosensitiveportion at one side of a substrate and an active CMOS or BICMOSelectronic circuit at an opposite side of the substrate, wherein: saidphotosensitive portion at one side of said substrate comprises at leastone photodetector comprising a P-doped region, an N-doped region, and anI-region of low doped or undoped semiconductor material that is betweenthe N-doped region and the P-doped region and has at least one holedeliberately formed to extend into said photosensitive portion; whereinsaid I-region is essentially single-crystal semiconductor materialhaving inherent crystal planes and said at least one hole extents intosaid photosensitive portion to a depth exceeding a depth of an invertedpyramid hole with sides along said crystal planes; said active circuitat an opposite side of said substrate comprises plural active electronicelements; connecting electrodes are configured to carry to said activeelectronic circuit electrical signals generated by said photosensitiveportion in response to illumination, for processing by said activeelectronic circuit; and output electrodes are connected to said activeelectronic circuit and are configured to deliver electrical signalsprocessed by the active electronic circuit.
 2. The structure of claim 1,in which said P-doped region, N-doped region, and I-region arevertically arranged.
 3. The structure of claim 2, in which said at leastone hole extends through one and toward the other of said P-doped regionand N-doped region.
 4. The structure of claim 3, further includingmaterial of one of said P-doped region and N-doped region at sidewallportions of said at least one hole.
 5. The structure of claim 2 in whichsaid I-region is at a closed end of said at least one hole and along atleast sidewall portions thereof.
 6. The structure of claim 2, in whichone of said P-doped region and N-doped region extends along at leastsidewall portions of said at least one hole.
 7. The structure of claim2, in which said at least one hole extends through said P-doped regionand N-doped region.
 8. The structure of claim 2, in which said at leastone hole comprises plural holes laterally spaced from each other andsaid photosensitive portion comprises plural photodetectors.
 9. Thestructure of claim 2, further including at least one avalanchephotodiode structure.
 10. The structure of claim 2, further including atleast one single photon avalanche photodiode (SPAD).
 11. The structureof claim 1, in which said P-doped region, N-doped region, and I-regionare laterally arranged.
 12. The structure of claim 11, in which one ofsaid P-doped region and N-doped region is at a closed end and atsidewall portions of said at least one hole.
 13. The structure of claim11, in which said at least one hole extends through at least one of saidP-doped region and N-doped region.
 14. The structure of claim 13, inwhich said at least one hole extends into both said P-doped region andN-doped region.
 15. The structure of claim 11, in which said at leastone hole penetrates through both said P-doped region and N-doped region.16. The structure of claim 11, in which said at least one hole comprisesplural holes laterally spaced from each other and said photosensitiveportion comprises plural photodetectors laterally spaced from eachother.
 17. The structure of claim 11, in which said at least one holehas a closed end at one of said P-doped region and N-doped region. 18.The structure of claim 11, further including at least one avalanchephotodiode structure.
 19. The structure of claim 11, further includingat least one single photon avalanche photodiode (SPAD).
 20. Anintegrated, single-chip structure comprising: I-regions of low-doped orundoped first semiconductor material that are laterally spaced from eachother by deliberately formed first holes extending in said firstsemiconductor material; regions of said first semiconductor materialdoped to one polarity; and regions of a second semiconductor materialthat is different from said first semiconductor material and comprisetriplets each formed of a region that is doped to an opposite polarityand is laterally between regions doped to said one polarity; whereinadjacent regions of said first semiconductor material are laterallyspaced from each other by said triplets of the second semiconductormaterial; wherein said I-regions and regions of said first semiconductormaterial doped to said one polarity and said regions of said secondsemiconductor material doped to an opposite polarity are configured asphotodetectors generating electrical signals in response toillumination, where illumination concurrently illuminating plural onesof said holes contributes to a respective single one of said electricalsignal; and wherein said regions of said second semiconductor materialare configured as avalanche structures.
 21. The structure of claim 20,further including first and second interdigitated electrodesrespectively coupled to said regions of the first semiconductor doped tosaid one polarity and to said regions of the second semiconductormaterial doped to said other polarity.
 22. The structure of claim 20, inwhich said regions of the first semiconductor doped to said oneconductivity are spaced vertically from said regions of the secondsemiconductor material.
 23. The structure of claim 20, further includingadditional deliberately formed holes in said first semiconductormaterial that are laterally between adjacent ones of said first holes.24. An integrated, single-chip structure comprising: an I-region oflow-doped or undoped Si semiconductor material; P-doped regions andN-doped regions extending in said semiconductor material; deliberatelyformed holes extending into said semiconductor material and laterallyspacing said doped regions; wherein each P-doped region is laterallyspaced from an adjacent N-doped region by at least one of said holes;and first and second interdigitated electrodes, respectively coupled tosaid P-doped regions to said N-doped regions; and wherein said structureis configured to generate an electrical signal in response to lightconcurrently impinging on a plurality of said holes to generate arespective common electrical output representing said light and tooperate at Gigahertz data rates.
 25. An integrated, single-chipstructure comprising: a first I-region of low-doped or undoped Ge orGe/Si alloy semiconductor material; a second I-region of low-doped orundoped Si semiconductor material; doped regions in said Ge or Ge/Simaterial that are doped to one polarity; doped regions in said Sisemiconductor material that are doped to opposite polarity and laterallyspace from each other said regions doped to said one polarity; holesdeliberately formed in said Ge or GeSi alloy material; and first andsecond interdigitated electrodes coupled respectively to said P-dopedregions and to said N-doped regions; and wherein said structure isconfigured to generate electrical signals in response to light and tooperate at Gigahertz data rates.
 26. An integrated, single-chipstructure comprising: an I-region of low-doped or undoped Ge or GeSialloy semiconductor material; P-doped regions and N-doped regionsextending in said semiconductor material; deliberately formed holesextending into said semiconductor material and laterally spacing saiddoped regions from each other; wherein each P-doped region is laterallyspaced from an adjacent N-doped region by at least one of said holes; alow-doped Si region extending along said Ge or GeSi region at a sidethereof opposite said doped regions; and first and second interdigitatedelectrodes coupled respectively to said regions doped to oneconductivity and to said regions doped to opposite conductivity; andwherein said structure is configured to generate electrical signals inresponse to light and to operate at Gigahertz data rates
 27. Anintegrated, single-chip structure comprising: I-regions of Sisemiconductor that are low-doped or undoped; first regions of said Sisemiconductor material doped to one polarity; and second regions of saidSi semiconductor material doped to opposite polarity and third regionsof said Si semiconductor material doped to said one polarity, saidsecond a third regions forming triplets each comprising one of saidsecond regions doped to opposite polarity and located laterally betweentwo of said second regions doped to said one polarity; wherein adjacentones of said first regions are laterally spaced from each other by atleast one or said triplets; deliberately formed holes extending intosaid I-regions, wherein a plurality of said holes is laterally betweeneach adjacent pair of one of said first regions and one of saidtriplets; wherein said I-regions and said second regions are configuredas photodetectors generating electrical signals in response toillumination, and said triplets are configured as avalanche structures.28. An integrated, single-chip structure comprising a photosensitiveportion at one side of a substrate and an active CMOS or BICMOSelectronic circuit that is at an opposite side of the substrate,wherein: said photosensitive portion at one side or of said substratecomprises plural sets of regions, each set comprising a P-doped region,an N-doped region, and an I-region of low doped or undoped semiconductormaterial that is between the N-doped region and the P-doped region;plural holes extend in said photosensitive regions and are laterallylocated between said sets; said active circuit at an opposite side ofsaid substrate comprises plural active electronic elements; first andsecond electrodes connect respectively said P-doped regions and saidN-doped regions and are configured to carry electrical signals generatedby said photosensitive portion in response to illumination to saidactive electronic circuit for processing; wherein at least two of saidsets are connected to combine the electrical signals they generate intoa common signal; and output electrodes are connected to said activeelectronic circuit and are configured to deliver electrical signalsprocessed by the active electronic circuit.
 29. The structure of claim28, in which each of said sets comprises a vertical stack of regions.30. The structure of claim 28, in which the regions of each of said setsare laterally spaced from each other.
 31. The structure of claim 28, inwhich said holes are arranged in an aperiodic array.